DSF-AI includes two distinct tools. This page documents what each has been tested against, and how honestly we can characterize each result.
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.
| Material | Known Transition | Type | Detected? | Precursor Lead |
|---|---|---|---|---|
| YBa2Cu3O7 | Tc = 93 K | High-Tc superconductor | Yes | 13 K |
| MgB2 | Tc = 39 K | Conventional superconductor | Yes | 18 K |
| CsV3Sb5 | Tc = 2.5 K | Kagome superconductor | Yes | — |
| VO2 | TMIT = 340 K | Metal-insulator | Yes | 20 K |
| BaTiO3 | TCurie = 393 K | Ferroelectric | Yes | 22 K |
| FeSe/STO | Tc = 65 K | Iron-based superconductor | Yes | 20 K |
| Pharma DSC | 5 transitions | DSC polymorph screening | 5 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.
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.
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.
| Cluster | Computed | Experiment | Error | Source |
|---|---|---|---|---|
| Fe13 | 2.500 | 2.500 | 0.0% | Knickelbein, PRL 86, 5255 (2001); T ≈ 120 K |
| Co13 | 2.000 | 2.000 | 0.0% | Xu & de Heer, PRL 106, 187202 (2011); T ≈ 78 K |
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.
| Cluster | Predicted | Experiment | Error | Source |
|---|---|---|---|---|
| Ni13 | 0.913 | 0.900 | 1.4% | Apsel et al., PRL 1996 |
| Fe55 | 2.40 | 2.4 | ~0% | Billas et al., Science 1994 |
| Co55 | 1.85 | 1.9 | 2.6% | Billas et al., Science 1994 |
| Ni55 | 0.75 | 0.75 | 0.0% | Apsel et al., PRL 1996 |
| Fe147 | 2.35 | 2.35 | ~0% | Billas et al., Science 1994 |
| Co147 | 1.78 | 1.8 | 1.1% | Billas et al., Science 1994 |
| Ni147 | 0.68 | 0.68 | 0.0% | Apsel et al., PRL 1996 |
| Fe700 | 2.25 | 2.25 | ~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.
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.
| Cluster | Predicted | Experiment | Error | Source |
|---|---|---|---|---|
| Au13 | 3.71 | 3.80 | 2.4% | Taylor et al., JCP 1992 |
| Au7 | 3.52 | 3.46 | 1.7% | Taylor et al., JCP 1992 |
| Au5 | 3.36 | 3.09 | 8.7% | Taylor et al., JCP 1992 |
| Ag13 | 2.69 | 2.50 | 7.6% | Ho et al., JCP 1990 |
| Ag7 | 2.38 | 2.40 | 0.8% | Ho et al., JCP 1990 |
| Cu13 | 2.94 | 2.85 | 3.2% | Ho et al., JCP 1990 |
| Ag8 | 2.85 | 1.60 | 78% | 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.
Computed from a proprietary geometric model. The calculation was performed before comparison to the published value.
| Cluster | Lattice | Predicted | Reference | Error | Source |
|---|---|---|---|---|---|
| Au13 | Cubic | +87.6 | +93 | 5.8% | 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.
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.
| Cluster | Predicted | Experiment | Error | Source |
|---|---|---|---|---|
| Au13 | 0.648 | 0.650 | 0.3% | Guvelioglu et al., PRL 2005 |
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.
| Element | Predicted | Bulk Measured | Match |
|---|---|---|---|
| Au | + | +1.94 μV/K | Yes |
| Ag | + | +1.51 | Yes |
| Cu | + | +1.83 | Yes |
| Pt | − | −5.28 | Yes |
| Ni | − | −19.5 | Yes |
| Co | − | −30.8 | Yes |
| Fe | + | +15.0 | Yes |
| Pd | − | −10.7 | Yes |
| Ta | − | −2.40 | Yes |
23/23 elements correct. Full table includes all 3d, 4d, and 5d transition metals.
If you've used DSF-AI on your own data and want to share your experience, contact support@dsf-ai.com.