Lilienfeld 1926 Stability Under Sustained Operation

# Characterize Stability Under Sustained Operation: The Fracture Margin Adds a Fourth Timeline

The 1925 protocol tracked three independent timescales of drift: operational (device under continuous bias), storage (unbiased shelf life), and cycling (repeated power on/off). This construction needs a fourth: whether the fracture-margin leakage component Step 8 identified as Path B grows over time as the Step 6 seal ages at that specific interface. Path B's magnitude is not guaranteed to stay fixed at whatever value Step 8 first measured — if the seal is slowly failing at the fracture margin specifically, rather than degrading uniformly across all four sealed interfaces, Path B will grow while the device's other characteristics remain stable, and only a timeline that isolates this one path will catch it.

Four Parallel Timelines, One Specific to This Geometry operational, storage, and cycling drift mirror 1925; fracture-margin drift does not Operational continuous bias Storage unbiased shelf Cycling power on/off Fracture-margin (new) seal aging at Path B Each timeline is tracked independently — a device can be stable on three and drifting on the fourth Only re-running Step 8's dwell-time fit at each checkpoint isolates fracture-margin drift from the others

The fracture-margin timeline requires a specific re-measurement, not a general health check. Operational, storage, and cycling drift can all be caught by periodically re-running Step 7's baseline I-V test — a general-purpose check. Fracture-margin drift requires re-running Step 8's specific dwell-time decay fit at each checkpoint, because only that measurement separates the decaying Path A component from the Path B plateau. A checkpoint that only re-measures baseline conductance could show a perfectly stable device while Path B silently grows underneath, because Path B's conduction only shows up distinctly in the control-electrode leakage measurement, not in the film's own terminal-to-terminal resistance.

Saturating exponential trend fitting applies here exactly as in the 1925 protocol, but to a different quantity. Where the 1925 series fit X(t) = X₀ + ΔX(1 − e^(−t/τ)) to baseline conductance and leakage drift, this construction fits the same functional form to the Step 8 plateau value itself, tracked across checkpoints. A growing plateau that saturates at some elevated value indicates a seal that is degrading toward a new, worse steady state rather than one that will continue degrading indefinitely — the same distinction the 1925 protocol drew between a bounded settling process and genuine ongoing failure.

Checkpoint Trend: Plateau Value Over Time re-fit Step 8's decay at each checkpoint; track whether the plateau itself drifts checkpoint number → plateau I₁₃ stable: no fracture-margin drift degrading: seal aging at Path B Checkpoint actions: Observation Interpretation Action Plateau flat across checkpoints seal holding at fracture margin continue schedule Plateau rises, then flattens settling to a new, worse state re-run Step 9 at new baseline Plateau rises without bound ongoing seal failure retire specimen, inspect seal
StepProcess operationInputOutputSpecificationConstraint
12.1Establish checkpoint schedule across all four timelinesReproducibility-confirmed population from Step 11Locked checkpoint scheduleCheckpoints spaced to resolve expected drift timescales; schedule fixed before monitoring beginsAdaptive checkpoint spacing based on early results undermines the pre-registration discipline used throughout this series
12.2At each checkpoint, re-run Step 7 baseline I-V testDevice from prior checkpointBaseline trend pointSame four-wire protocol and settling discipline as original Step 7Deviating from the original test procedure introduces a confound separate from genuine drift
12.3At each checkpoint, re-run Step 8 dwell-time decay fitDevice from prior checkpointτ and plateau I₁₃ trend pointSame bias magnitude and dwell duration as original Step 8A different bias magnitude at checkpoint time changes the comparison basis for Path B's plateau value
12.4Fit saturating exponential to each of the four timeline's checkpoint seriesTrend points from 12.2, 12.3, and operational/storage/cycling logsFour independent trend fitsX(t) = X₀ + ΔX(1 − e^(−t/τ_trend)) fit to each seriesFitting a single combined trend across all four timelines would mask which specific mechanism is drifting
12.5Compare each ΔX against the repeatability bounds established in Steps 7 and 8Trend fits from 12.4Pass/fail per timelineΔX within original measurement repeatability counts as stable; beyond it counts as driftUsing an arbitrary drift threshold instead of the device's own measured repeatability bound invites inconsistent judgment across specimens
12.6For any timeline showing drift, determine whether the trend has saturated or is still risingPass/fail results from 12.5Drift classification: settled vs. ongoingSaturated trend (flattening ΔX) classified separately from unbounded rising trendTreating all drift as equally severe ignores the practical difference between settling to a new stable state and ongoing failure
12.7For fracture-margin drift specifically, cross-check against Step 6.7's original pre-seal and post-seal resistance valuesFracture-margin trend from 12.6Seal-degradation root-cause estimateCompare current plateau trajectory against the gap (if any) already present between Step 6.7's before/after valuesA device that already showed a small gap at Step 6.7 is a better candidate for eventual fracture-margin drift than one that showed none
12.8Record final stability classification per device, per timeline, with supporting trend fitsAll prior resultsComplete stability characterization recordAll four timelines reported individually; no single combined "stability" verdict that obscures which mechanism is responsibleA single pass/fail stability number discards exactly the diagnostic structure this four-timeline approach was built to preserve

Step 12 is where the population-level reproducibility result from Step 11 gets a time dimension. A construction method that reproduces well at a single point in time (Step 11) but drifts unpredictably at the fracture margin over weeks or months is not yet a trustworthy construction — it is one whose failure mode has simply not yet had time to appear. Tracking the fracture-margin timeline separately from the three mechanisms the 1925 protocol already tracked is what lets this distinction surface before it becomes an unexplained field failure.

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