LK-99
Nothing yet separates the substituted apatite from other phases and artifacts.
- claims
- 6
- holes
- 6
- lenses
- 3
- records cited
- 5 of 14
- retracted precedents
- 0
What happened, 16 August 2023. Nature reports the impurity explanation. Within weeks, replication work found no superconductivity. A copper sulfide impurity, which changes phase near 104 °C, explained the jump in resistivity; ordinary diamagnetism or ferromagnetism explained the partial levitation; pure single crystals were insulators (August 2023). The model writing the review knew how it ended.
The idea, as it stood
We have synthesised a modified lead apatite in which copper replaces some of the lead. We measure superconductivity with a critical temperature of at least 400 K (127 °C) at ambient pressure. We attribute it to a small structural distortion: the copper substitution shrinks the volume slightly, which we believe creates the conditions for superconductivity. We plan to announce it as the first room-temperature, ambient-pressure superconductor.
- The synthesised material is a lead apatite in which copper has replaced part of the lead.empirical · supported
- The measured signal is superconductivity arising in the copper-substituted apatite phase itself, at ambient pressure.empirical · contested · it breaks here
- The superconducting critical temperature is at least 400 K (127 °C).empirical · unsupported
- Copper substitution slightly shrinks the lattice volume, producing a small structural distortion.empirical · supported
- That volume shrinkage and distortion is what creates the conditions for superconductivity.causal · unsupported
- The result is strong enough to announce as the first room-temperature, ambient-pressure superconductor.normative · unsupported
The holes, and who found them
More than one lens found a hole in claim 2, each on its own. That is a stronger signal than one lens alone.
| # | Hole | Lens | How serious | Claim | Status |
|---|---|---|---|---|---|
| 1 | Nothing yet separates the substituted apatite from other phases and artifacts | Richard Feynman | fatal | 2 | Open |
| 2 | The 400 K claim names no transition and no result that would refute it | Karl Popper | fatal | 3 | Open |
| 3 | Announced before anyone has tried to refute it, with 'first' already in question | Karl Popper | serious | 6 | Open |
| 4 | An average over the sample hides which grains and batches carry the signal | Barbara McClintock | serious | 2 | Open |
| 5 | 'Creates the conditions' names a correlation, not a mechanism | Richard Feynman | serious | 5 | Open |
| 6 | A 0.48% shrinkage is small enough to need a same-route control | Richard Feynman | minor | 4 | Open |
What it rests on
- The First Room-Temperature Ambient-Pressure SuperconductorLee et al. · 2023 · arXiv (Cornell University) · cited on claim 2, 3, 4, 5, 6 · doi:10.48550/arxiv.2307.12008
- Single Crystal Growth Tricks and TreatsTanya et al. · 2022 · arXiv (Cornell University) · cited on claim 2 · doi:10.48550/arxiv.2209.09370
- Oxide Room Temperature Superconductivity At Ambient Pressure: Computations and Experimental VerificationsIsikaku-Ironkwe · 2021 · Bulletin of the American Physical Society · cited on claim 6 · record
- Room-Temperature Superconductivity in Yb/Lu Substituted Clathrate Hexahydrides under Moderate PressureDu et al. · 2022 · Research · cited on claim 6 · doi:10.34133/2022/9784309
- The 2021 room-temperature superconductivity roadmapBoeri et al. · 2021 · Journal of Physics Condensed Matter · cited on claim 6 · doi:10.1088/1361-648x/ac2864
- On the practical limits to substitutionAyres · 2006 · Ecological Economics · retrieved, not cited · doi:10.1016/j.ecolecon.2006.02.011
- Study of the mechanisms of heavy metal sorption by mineral apatite: the feasibility of soil and ground water remediationRadoičić · 2010 · retrieved, not cited · doi:10.2298/bg20101005kaludjerovicradoicic
- From Cu2S nanocrystals to Cu doped CdS nanocrystals through cation exchange: controlled synthesis, optical properties and their p-type conductivity researchLiu et al. · 2015 · Science China Materials · retrieved, not cited · doi:10.1007/s40843-015-0080-z
- COMPILATION OF CRYSTAL GROWERS AND CRYSTAL GROWTH PROJECTS.Zoology & Connolly · 1972 · retrieved, not cited · doi:10.2172/4624081
- Separation of Ag and Cu from Their Aqueous Thiosulfate Complexes by UV-C IrradiationHan et al. · 2019 · Metals · retrieved, not cited · doi:10.3390/met9111178
- Modularity and Twinning in Mineral Crystal StructuresFerraris · 2021 · MDPI eBooks · retrieved, not cited · doi:10.3390/books978-3-0365-1916-6
- Anion substitution in Perovskite related materials for fuel cell applicationsHancock · 2012 · University of Birmingham Institutional Research Archive (University of Birmingham) · retrieved, not cited · record
- Chemo-sensors development based on low-dimensional codoped Mn2O3-ZnO nanoparticles using flat-silver electrodesRahman et al. · 2013 · Chemistry Central Journal · retrieved, not cited · doi:10.1186/1752-153x-7-60
- Synthèse par ammonolyse et étude des propriétés de luminescence dans des oxynitrures de structure apatite dopés au cérium ou à l’europiumThomas · 2012 · HAL · retrieved, not cited · doi:10.70675/dcd28896zcfe1z4903zab71z21976b0f3f04
The tests that settle it
The deciding test · weeks of work
Quantify every phase in the sample you measured. Then, on that sample and on material with its secondary phases removed or reduced (or a single crystal), measure four-probe resistance and zero-field-cooled and field-cooled magnetization from room temperature to well above the claimed transition, on heating and cooling, under several applied magnetic fields.
It fails if: In the purer material, resistance does not fall to the instrument floor at the same temperature that flux expulsion appears; or that temperature does not move down under applied field; or zero-field-cooled shielding covers far less of the sample than the apatite's measured volume fraction; or the step shows heating-cooling hysteresis beyond the setup's thermal lag; or the signals weaken as the secondary phases are removed.
| For hole | Test | Result |
|---|---|---|
| 1 | Quantify every phase in the measured samples by refined X-ray or neutron diffraction and by electron microscopy with elemental mapping. Then measure four-probe resistance and zero-field-cooled and field-cooled magnetization on phase-pure substituted apatite or single crystals (E3 reviews growth routes used for defect control), and on samples deliberately enriched in each secondary phase found. Counts against the idea: the resistance drop or the diamagnetic signal weakens or vanishes as phase purity rises, or scales with a secondary-phase fraction rather than with the apatite. | Proposed |
| 2 | Before measuring, state the transition temperature and the refuting results. Then, on one sample, from room temperature to well above the transition, on heating and cooling, measure four-probe resistance with the instrument floor stated and a copper sample of the same geometry as reference, zero-field-cooled and field-cooled magnetization, and the resistive transition under several applied fields and currents. Counts against the idea: resistance below the transition stays measurably above the floor; the transition does not shift or broaden with field or current; field cooling shows no flux expulsion; the resistive and magnetic transitions fall at different temperatures; or the step shows hysteresis between heating and cooling larger than the setup's thermal lag, the mark of a first-order structural change rather than a zero-field superconducting transition. | Proposed |
| 3 | Before any announcement, give samples, unsubstituted controls and the complete recipe (precursors, temperatures, atmospheres, durations) to at least two independent laboratories, and have them measure four-probe resistance and zero-field-cooled and field-cooled magnetization through the claimed transition without knowing which samples are which. Separately, collect every published attempt since 2023 to reproduce the material in E2 and compare it with your data. Counts against announcing: the independent laboratories do not obtain zero resistance together with flux expulsion from the recipe, or published reproductions of E2's material find no superconductivity. | Proposed |
| 4 | Make several batches independently and cut each into fragments. For every fragment, record the resistance or magnetic response and, on the same fragment, the phases present and the local copper content by electron microscopy with elemental mapping; repeat the response measurement after cycling each fragment through the transition several times. Counts against the idea: the response appears only in fragments containing a particular non-apatite phase, shows no relation to the copper content of the apatite, or fades or shifts with cycling. | Proposed |
| 5 | Turn the mechanism into a prediction. Make a series with different copper fractions; for each, refine the lattice volume and the Pb(2) site geometry and measure the transition. Add two controls: unsubstituted lead apatite compressed hydrostatically until its measured volume shrinks by the same amount, and an apatite carrying a different small divalent substituent that gives a similar shrinkage. Counts against the claim: the transition does not track the measured shrinkage across the series, or superconductivity appears only when copper is present, whatever the shrinkage. | Proposed |
| 6 | Make unsubstituted and substituted apatite by the same route, measure both with an internal diffraction standard, refine the lattice parameters with their uncertainties, and repeat on several batches. Counts against the claim: the volume difference is within the batch-to-batch scatter of the unsubstituted control, or does not grow with copper content. | Proposed |
Proposed tests that haven’t run are the agenda for what comes next. Download them as a draft pre-registration, ready to edit and register on OSF.
The finding
Nothing in the evidence supplied refutes it, but nothing described yet separates superconductivity in the copper-substituted apatite from a secondary phase, an artifact or ordinary magnetism, and the only matching record (E2) restates the same claim with no independent replication.
It failed: Nature reports the impurity explanation. What would overturn the review’s reading: In the purer material, resistance does not fall to the instrument floor at the same temperature that flux expulsion appears; or that temperature does not move down under applied field; or zero-field-cooled shielding covers far less of the sample than the apatite's measured volume fraction; or the step shows heating-cooling hysteresis beyond the setup's thermal lag; or the signals weaken as the secondary phases are removed.
Cite it, disclose it, reproduce it
A paragraph for your methods section
We used Feynman (feynman.works), an AI research-review tool running on Claude Opus 5.5, to critique “LK-99” on 2026-11-01 (run agents-2026-11-01/superconductor). It reconstructed 6 claims, retrieved 14 published records dated no later than 2023-07-22, and raised 6 objections through reasoning frameworks drawn from the published work of Richard Feynman, Barbara McClintock and Karl Popper. Each citation in its output was checked against the records it retrieved, and we read every source we relied on. Its objections informed our analysis; the conclusions, and any errors, are our own.
The lenses
- Richard FeynmanPhysics & scientific method · 1948–1980What experiment would distinguish this explanation from a convincing story?
- Barbara McClintockGenetics & observation · 1931–1980What does the exception reveal that the average has hidden?
- Karl PopperPhilosophy of science · 1934–1980What conceivable observation would count against this claim?
BibTeX
@misc{feynman-agents-2026-11-01-superconductor,
title = {{Feynman review: LK-99}},
author = {{Feynman Works}},
year = {2026},
howpublished = {\url{https://www.feynman.works/pack/superconductor}},
note = {Run agents-2026-11-01/superconductor, Claude Opus 5.5, 2026-11-01}
}
@article{lee2023first,
title = {{The First Room-Temperature Ambient-Pressure Superconductor}},
author = {Lee and others},
year = {2023},
journal = {arXiv (Cornell University)},
doi = {10.48550/arxiv.2307.12008}
}
@article{tanya2022single,
title = {{Single Crystal Growth Tricks and Treats}},
author = {Tanya and others},
year = {2022},
journal = {arXiv (Cornell University)},
doi = {10.48550/arxiv.2209.09370}
}
@article{isikaku2021oxide,
title = {{Oxide Room Temperature Superconductivity At Ambient Pressure: Computations and Experimental Verifications}},
author = {Isikaku-Ironkwe},
year = {2021},
journal = {Bulletin of the American Physical Society},
url = {https://meetings.aps.org/Meeting/MAR21/Session/L47.14}
}
@article{du2022room,
title = {{Room-Temperature Superconductivity in Yb/Lu Substituted Clathrate Hexahydrides under Moderate Pressure}},
author = {Du and others},
year = {2022},
journal = {Research},
doi = {10.34133/2022/9784309}
}
@article{boeri2021room,
title = {{The 2021 room-temperature superconductivity roadmap}},
author = {Boeri and others},
year = {2021},
journal = {Journal of Physics Condensed Matter},
doi = {10.1088/1361-648x/ac2864}
}Run agents-2026-11-01/superconductor on Claude Opus 5.5. The review is reproducible from its record: the claims, the records retrieved before 22 July 2023, and each lens’s card. https://www.feynman.works/pack/superconductor