DSF-AI

Validation Evidence

DSF-AI includes two distinct tools. This page documents what each has been tested against, and how honestly we can characterize each result.

Two tools, one brand. DSF Structural Analyzer runs the structural analysis engine on any two-column time series (R(T), DSC, impedance, etc.) to detect transitions and precursors. Nanoparticle Property Predictor predicts magnetic moments, electron affinities, Seebeck coefficients, and HOMO-LUMO gaps from element identity and cluster size alone. These are different computations under the same service.
How to read this page. Each result is labeled: Calibration = the experimental value informed the formula (not a blind prediction). Prediction = computed before comparison to experiment. Textbook = follows from known physics; confirms the formula encodes established trends, not that it discovered them.

DSF Structural Analyzer Phase Transition Detection

The analyzer was run on digitized R(T), resistivity, dielectric, and DSC data from published papers. All transitions were known beforehand — this tests whether the analyzer finds them, not whether they're new.

MaterialKnown TransitionTypeDetected?Precursor Lead
YBa2Cu3O7Tc = 93 KHigh-Tc superconductorYes13 K
MgB2Tc = 39 KConventional superconductorYes18 K
CsV3Sb5Tc = 2.5 KKagome superconductorYes
VO2TMIT = 340 KMetal-insulatorYes20 K
BaTiO3TCurie = 393 KFerroelectricYes22 K
FeSe/STOTc = 65 KIron-based superconductorYes20 K
Pharma DSC5 transitionsDSC polymorph screening5 of 5

Same pipeline, same parameters across all domains tested. The pipeline was developed against financial time series; subsequent applications to materials and pharmaceutical data used identical code and parameters. Click material names for full case studies. Try it on your data.

The precursor leads (13–22 K before the known transition) are the most interesting finding — the analyzer detects changes in the data before the transition is conventionally visible. Whether these correspond to real physical precursors (e.g., superconducting fluctuations above Tc) requires independent experimental confirmation.

Nanoparticle Property Predictor Predictions

The predictor uses a proprietary geometric framework and tabulated physical constants (NIST, CRC Handbook). It does NOT use the structural analysis engine. Results below are categorized by how they were obtained.

Magnetic Moments (μB/atom)

Framework-Informing Data Calibration

The magnetic moment formula was calibrated using Fe13 and Co13 experimental values. These results confirm the formula is correct for the data that informed it — they are not independent predictions.

ClusterComputedExperimentErrorSource
Fe132.5002.5000.0%Knickelbein, PRL 86, 5255 (2001); T ≈ 120 K
Co132.0002.0000.0%Xu & de Heer, PRL 106, 187202 (2011); T ≈ 78 K

Genuine Predictions Prediction

Ni13 uses a pair correction derived from the geometric framework using tabulated spin-orbit and Stoner constants. This correction was not fitted to Ni's value. The size-dependent predictions (N=55, 147, 700) extrapolate using standard size-scaling physics, not a fit.

ClusterPredictedExperimentErrorSource
Ni130.9130.9001.4%Apsel et al., PRL 1996
Fe552.402.4~0%Billas et al., Science 1994
Co551.851.92.6%Billas et al., Science 1994
Ni550.750.750.0%Apsel et al., PRL 1996
Fe1472.352.35~0%Billas et al., Science 1994
Co1471.781.81.1%Billas et al., Science 1994
Ni1470.680.680.0%Apsel et al., PRL 1996
Fe7002.252.25~0%Billas et al., Science 1994

Note: The magnetic moment formula was calibrated at N=13 for Fe and Co. Its predictions at larger sizes (Fe55, Fe147, Fe700) test whether the size-scaling is correct. The Ni pair correction uses tabulated constants from NIST and was not fitted to Ni's experimental value.

Electron Affinity (eV) Prediction

Uses the Perdew metallic sphere model (textbook electrostatics) applied to cluster geometry, plus a Kubo gap correction for odd/even electron count. The model existed before we applied it — these are predictions from a known model applied to specific cluster sizes.

ClusterPredictedExperimentErrorSource
Au133.713.802.4%Taylor et al., JCP 1992
Au73.523.461.7%Taylor et al., JCP 1992
Au53.363.098.7%Taylor et al., JCP 1992
Ag132.692.507.6%Ho et al., JCP 1990
Ag72.382.400.8%Ho et al., JCP 1990
Cu132.942.853.2%Ho et al., JCP 1990
Ag82.851.6078%Ho et al., JCP 1990

Known failure: Ag8 is a non-magic cluster size (between geometric shell closings). The metallic sphere model breaks for N < 10–12 atoms, where quantum shell effects dominate over classical electrostatics. The predictor is reliable at magic numbers (13, 55, 147) and degrades at small non-magic sizes.

Seebeck Coefficient (μV/K) Prediction

Computed from a proprietary geometric model. The calculation was performed before comparison to the published value.

ClusterLatticePredictedReferenceErrorSource
Au13Cubic+87.6+935.8%Kurelchuk et al., 2019

240 additional predictions available for all 23 d-metals. These are untested predictions — no experimental comparison exists for most of them. Try the screener.

HOMO-LUMO Gap (eV) Consistent with measurement

Derived from tabulated spin-orbit constants via the geometric framework. The formula produces the correct value from atomic constants; the timeline of computation vs. literature comparison was not recorded.

ClusterPredictedExperimentErrorSource
Au130.6480.6500.3%Guvelioglu et al., PRL 2005

Seebeck Sign Predictions Textbook

The sign rule (d-band filling determines Seebeck sign) follows from established electronic structure theory. The 23/23 result confirms the formula correctly encodes known d-band physics — it does not represent a discovery. Full and half-filled d-shells have well-known transport asymmetries.

ElementPredictedBulk MeasuredMatch
Au++1.94 μV/KYes
Ag++1.51Yes
Cu++1.83Yes
Pt−5.28Yes
Ni−19.5Yes
Co−30.8Yes
Fe++15.0Yes
Pd−10.7Yes
Ta−2.40Yes

23/23 elements correct. Full table includes all 3d, 4d, and 5d transition metals.

What Would Strengthen This

Current limitations

What would strengthen this

If you've used DSF-AI on your own data and want to share your experience, contact support@dsf-ai.com.