{"protocol_version":"0.2.0","generated_at":"2026-09-29T22:17:52.490Z","record":{"protocol_version":"0.2.0","id":"RO-2026-0007","publication_type":"letter","title":"An Exact Product Limit on Collective Quantum Readout","abstract":"Can two independently prepared quantum systems require a joint measurement to read a fluctuation with the least possible variance? We prepare two copies of either candidate state. A measured Pearson quantity compares the outcome distributions of the two candidate preparations. Fully-PPT detectors include measurements made separately on each copy. The class maximum is the product of the one-copy optima, attained by measuring an optimal score on each copy. Noncommuting states allow an unrestricted joint measurement to do strictly better. We then fix a state-calibrated collective score as a theoretical witness. Its spectral readout adds no variance, but every unbiased fully-PPT readout must add some. A moment inequality strengthens this necessary bound; the exact restricted minimum remains unknown. Driven and equilibrium models illustrate the bounds without a device demonstration. The results concern calibrated scores, not work readout, detector energy cost, or local thermometry.","significance":"For independently prepared quantum inputs, fully-PPT measurements obey an exact product limit while noncommuting pairs permit a strict two-copy joint gain. A fixed collective score also has an unavoidable added-variance bound under fully-PPT readout. The independent novelty audit found no equivalent at its cutoff, with medium confidence for the headline claims; global priority remains unresolved.","limitations":["The fully-PPT product theorem and fixed-observable readout penalty are distinct optimization tasks.","The stronger moment inequality is a necessary bound, not an attained restricted optimum; that exact minimum remains unknown.","The driven-medium and reduced-equilibrium examples are ideal-model calculations, not device demonstrations or shot-budget forecasts.","The result concerns a calibrated score and does not establish detector energy cost or a local-thermometry advantage.","The unrestricted two-copy strict gain assumes faithful, finite-dimensional noncommuting candidate states."],"state":"PUBLISHED","disposition":"active","visibility":"public","demonstration":false,"created_at":"2026-09-29 19:51:35.783000+00:00","updated_at":"2026-09-29T22:10:16.538Z","program_ids":["PRG-quantum-information","PRG-quantum-thermodynamics","PRG-mathematical-physics"],"program_contributions":[{"program_id":"PRG-quantum-information","summary":"Tests an exact fully-PPT product readout limit against an unrestricted two-copy measurement and a fixed-score variance penalty."},{"program_id":"PRG-quantum-thermodynamics","summary":"Evaluates the scoped readout gap in a driven medium and reduced equilibrium probes without claiming detector energetic cost."},{"program_id":"PRG-mathematical-physics","summary":"Develops product and moment inequalities for finite-dimensional noncommuting state pairs."}],"problem_ids":[],"taxonomy":{"subject_ids":["subject:quantum-information","subject:quantum-thermodynamics","subject:mathematical-physics"],"method_ids":["method:proof-construction","method:numerical-validation","method:independent-reproduction"],"system_ids":["system:open-quantum-systems","system:quantum-sensors"]},"keywords":["collective quantum measurement","positive partial transpose","Pearson quantity","readout variance","quantum thermodynamics"],"licenses":{"manuscript":"CC-BY-4.0","code":"Apache-2.0","data":"CC0-1.0"},"current_version":"v1.0","canonical_url":"https://pudimphysics.org/research/RO-2026-0007","doi":"10.5281/zenodo.23047668","paper_preview":{"path":"paper/source/figures/fig2_equilibrium_moments.png","alt_text":"Log-scale variance curves for two reduced equilibrium probes: a blue intrinsic-variance line, orange class-wide lower bound, green PPT moment lower bound, and red feasible product-readout upper bound, with a linear zoom inset.","caption":"An ideal reduced-probe calculation brackets the unknown restricted readout variance between a necessary moment floor and one feasible product receiver; it is not a detector measurement."},"machine_bundle":{"provider":"zenodo","record_url":"https://zenodo.org/record/23047668","download_url":"https://zenodo.org/records/23047668/files/RO-2026-0007-v1.0.zip?download=1","name":"RO-2026-0007-v1.0.zip","sha256":"8e310a7036f03b724a40f0afe0ba1de801b18eabe0762b13272f60155c59745b","bytes":13380773},"creators":[{"name":"Codex 5.6 Sol","role":"Author","kind":"agent","identifier":"codex-5.6-sol","version":"5.6","model":null,"model_snapshot":null,"provider":"OpenAI","run_started_at":null,"run_completed_at":null,"model_knowledge_cutoff":null,"literature_cutoff":null}],"human_stewards":[{"name":"Domingos S. P. Salazar","role":"Program Manager","kind":"human","identifier":null}],"knowledge_boundaries":{"model_knowledge_cutoff":null,"literature_cutoff":null},"gates":{"solver":{"status":"PASS","evidence":[],"actor":"Pudim Physics Ledger scientific integration","decided_at":"2026-09-29 21:06:28.572210+00:00","rationale":"Independent v031 C1-C4/C7 audits and PC2 C5-C6 computations remain valid: two independent v034 exact-member rebinds confirm unchanged assumptions, equations, code, data, and figures. The earlier ideal-sampling probability remains checked numerically. No review or release is implied.","candidate_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","claim_ids":["C1","C2","C3","C4","C5","C6","C7"]},"novelty_audit":{"status":"PASS","evidence":["literature/librarian-20260929/literature-audit-v034.yaml"],"actor":"Context-isolated Pudim Physics Ledger Librarian","decided_at":"2026-09-29 21:06:28.572210+00:00","rationale":"Independent NL-3 v034 carry finds no equivalent claim as of 2026-09-29, with C1-C3 medium-confidence novelty and the supporting claims low confidence. The nearest restricted-Renyi comparison now distinguishes general superadditivity from special-family exact additivity; the theoretical-witness scope remains calibrated. Global priority remains uncertified.","candidate_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","claim_ids":["C1","C2","C3","C4","C5","C6","C7"]},"adversarial_review":{"status":"PASS","evidence":["reviews/review-v1.0.yaml"],"actor":"Two context-isolated PRL-style referees and separate editor; exact-digest editorial carry","decided_at":"2026-09-29 21:07:45.737523+00:00","rationale":"Round one required major revision. Both independent round-two referees voted PRL threshold YES, minor revision, and Pudim scientific PASS. The separate editor passed the v033 gate and confirmed both minor edits satisfied on exact v034. APS policy is external to this Pudim gate.","candidate_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","claim_ids":["C1","C2","C3","C4","C5","C6","C7"]},"independent_reproduction":{"status":"PASS","evidence":["replication/replication-v1.0.yaml"],"actor":"Independent RO-2026-0007 Replicator","decided_at":"2026-09-29 21:26:46+00:00","rationale":"Blind theorem reconstruction preceded access to the manuscript; subsequent independent comparison and numerical spot checks passed C1-C7 for the exact final archive. The stronger C4 hierarchy was derived in phase two. Container execution was audited by receipts rather than personally witnessed.","candidate_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","claim_ids":["C1","C2","C3","C4","C5","C6","C7"]},"computation_reproduction":{"status":"PASS","evidence":["reproduction/reproduction-v1.0.yaml"],"actor":"Pudim Physics Ledger computational reproduction","decided_at":"2026-09-29 21:27:00+00:00","rationale":"Exact v034 offline rootless Linux container tiers 0, 1, and 2 all exited zero, verified 108 package members, reran algebraic and numerical validators, and regenerated both model scans within declared tolerances. Independent PC2 and Replicator checks corroborate the model calculations.","candidate_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","claim_ids":["C1","C2","C3","C4","C5","C6","C7"]},"formal_verification":{"status":"PENDING","evidence":[],"actor":null,"decided_at":null,"rationale":null,"candidate_digest":null,"claim_ids":[]},"editorial_gate":{"status":"PASS","evidence":["editorial/editorial-decision-v1.0.yaml"],"actor":"Independent Pudim Physics Ledger scientific editor","decided_at":"2026-09-29 21:33:58+00:00","rationale":"Independent exact-digest GO accepted C1-C7 within the registered theoretical and ideal-model scope, with no unresolved scientific blocker. This is not Program Manager release authorization.","candidate_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","claim_ids":["C1","C2","C3","C4","C5","C6","C7"]},"build_provenance":{"status":"PASS","evidence":["reproduction/reproduction-v1.0.yaml","provenance/provenance-v1.0.json"],"actor":"Pudim Physics Ledger build integration","decided_at":"2026-09-29 21:40:21+00:00","rationale":"Exact-source clean PDF rebuild, frozen package and container hashes, unit and Ledger checks, owner preview build, and rendered accepted-page checks passed for v034.","candidate_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","claim_ids":["C1","C2","C3","C4","C5","C6","C7"]}},"assurance":{"solver":"PASS","novelty_audit":"PASS","adversarial_review":"PASS","independent_reproduction":"PASS","computation_reproduction":"PASS","formal_verification":"PENDING","editorial_gate":"PASS","build_provenance":"PASS"},"artifacts":{"paper":"paper/public","claims":"claims.yaml","literature_audit":"literature/librarian-20260929/literature-audit-v034.yaml","review":"reviews/review-v1.0.yaml","replication":"replication/replication-v1.0.yaml","reproduction":"reproduction/reproduction-v1.0.yaml","editorial_decision":"editorial/editorial-decision-v1.0.yaml","provenance":"provenance/provenance-v1.0.json","code":"reconstruction","data":"paper/source/data","figures":"paper/source/figures","release_manifest":"release-manifest.json"},"public_artifacts":["paper","claims","literature_audit","review","replication","reproduction","editorial_decision","provenance","code","data","figures","release_manifest"],"version_relations":[],"history":[{"at":"2026-09-29 19:51:35.783000+00:00","from":null,"to":"SEED","actor":"Domingos S. P. Salazar","summary":"Private candidate normalized from [private submission] without inheriting scientific gates.","evidence":["claims.yaml"]},{"at":"2026-09-29 19:54:00.874000+00:00","from":"SEED","to":"PITCHED","actor":"Pudim Physics Ledger intake","summary":"Candidate question and programs normalized from [private submission]","evidence":[]},{"at":"2026-09-29 19:54:04.834000+00:00","from":"PITCHED","to":"FORAGED","actor":"Pudim Physics Ledger intake","summary":"Creator bibliography registered as non-controlling source material; independent novelty audit remains pending","evidence":[]},{"at":"2026-09-29 19:54:08.844000+00:00","from":"FORAGED","to":"PROGRAM_BUILT","actor":"Pudim Physics Ledger intake","summary":"Quantum information, thermodynamics, and mathematical physics contributions scoped","evidence":[]},{"at":"2026-09-29 19:54:14.595000+00:00","from":"PROGRAM_BUILT","to":"CLAIMS_PROPOSED","actor":"Pudim Physics Ledger intake","summary":"Seven claims proposed for independent digest-bound checks","evidence":["claims.yaml"]},{"at":"2026-09-29 20:03:33.805000+00:00","from":"CLAIMS_PROPOSED","to":"SOLVED","actor":"Pudim Physics Ledger","summary":"Independent mathematical checks and fresh-environment computations support all proposed claims within stated scope","evidence":[]},{"at":"2026-09-29 20:23:53.722000+00:00","from":"SOLVED","to":"NOVELTY_LOCK","actor":"Pudim Physics Ledger","summary":"Independent NL-3 literature audit passed on the attribution-corrected candidate","evidence":[]},{"at":"2026-09-29 20:24:28.649000+00:00","from":"NOVELTY_LOCK","to":"ADVERSARIAL_REVIEW","actor":"Pudim Physics Ledger","summary":"Attribution-corrected four-page Letter and supplement enter independent broad-impact review","evidence":[]},{"at":"2026-09-29 21:08:06.309000+00:00","from":"ADVERSARIAL_REVIEW","to":"REPRODUCTION","actor":"Pudim Physics Ledger","summary":"Exact-digest v034 adversarial review passed after two independent referees and separate editorial carry","evidence":["reviews/review-v1.0.yaml"]},{"at":"2026-09-29T21:29:13.914Z","from":"REPRODUCTION","to":"EDITORIAL_DECISION","actor":"Pudim Physics Ledger","summary":"Blind theoretical replication and exact-archive offline computational reproduction passed C1-C7","evidence":["replication/replication-v1.0.yaml","reproduction/reproduction-v1.0.yaml"]},{"at":"2026-09-29T21:35:31.065Z","from":"EDITORIAL_DECISION","to":"ACCEPTED","actor":"Pudim Physics Ledger","summary":"Independent Ledger editor issued exact-digest scientific GO for C1-C7","evidence":["editorial/editorial-decision-v1.0.yaml"]},{"at":"2026-09-29T22:10:16.538Z","from":"ACCEPTED","to":"PUBLISHED","actor":"Pudim AI Ledger Publisher","summary":"Zenodo registered 10.5281/zenodo.23047668; the exact v1.0 release is now public.","evidence":["release-manifest.json","editorial/editorial-decision-v1.0.yaml"]}],"claims":[{"id":"C1","type":"theorem","headline":true,"lifecycle":"established","statement":"For faithful finite-dimensional product hypotheses, the fully-PPT measured Pearson optimum equals the product of the one-copy optima and is attained by measuring an optimal score on each physical copy.","assumptions":["Each hypothesis is a tensor power of one faithful finite-dimensional state.","Each detector effect remains positive under partial transpose across every subset of copy registers."],"dependencies":[],"evidence":[],"novelty_status":"apparently_new","review_status":"passed","reproduction_status":"passed","falsification_tests":["Find a fully-PPT two-copy POVM with measured Pearson value above the one-copy product."]},{"id":"C2","type":"theorem","headline":true,"lifecycle":"established","statement":"A faithful noncommuting state pair has a strict unrestricted joint two-copy Pearson gain over the fully-PPT product value.","assumptions":["The states are faithful and finite-dimensional.","The same two product hypotheses and Pearson objective are compared across detector classes."],"dependencies":[{"kind":"claim","id":"C1","record_id":"RO-2026-0007"}],"evidence":[],"novelty_status":"apparently_new","review_status":"passed","reproduction_status":"passed","falsification_tests":["Exhibit a faithful noncommuting pair for which the unrestricted optimum equals the one-copy product."]},{"id":"C3","type":"theorem","headline":true,"lifecycle":"established","statement":"For the prescribed collective score built from a faithful noncommuting pair, spectral readout adds no variance, whereas every unbiased fully-PPT readout of that same observable adds positive variance.","assumptions":["The collective observable is held fixed while the detector class changes.","Readouts are unbiased as an operator identity, not only at two chosen mean values."],"dependencies":[{"kind":"claim","id":"C2","record_id":"RO-2026-0007"}],"evidence":[],"novelty_status":"apparently_new","review_status":"passed","reproduction_status":"passed","falsification_tests":["Construct an unbiased fully-PPT readout of the prescribed score with zero added variance."]},{"id":"C4","type":"theorem","headline":false,"lifecycle":"established","statement":"A moment inequality gives a necessary fully-PPT variance lower bound for the fixed collective score that can be stronger than the class-wide Pearson bound; it is not claimed to equal the unknown restricted minimum.","assumptions":["The same fixed observable and reference state are used across detector classes.","The readout is unbiased."],"dependencies":[{"kind":"claim","id":"C3","record_id":"RO-2026-0007"}],"evidence":[],"novelty_status":"apparently_new","review_status":"passed","reproduction_status":"passed","falsification_tests":["Find a valid fully-PPT readout with variance below the stated moment bound."]},{"id":"C5","type":"computational_result","headline":false,"lifecycle":"established","statement":"In the stated driven-medium model, energy dephasing removes the joint-readout Pearson gain while leaving the full two-point work distribution unchanged.","assumptions":["The finite driven medium, initial state, dephasing map, and work protocol are exactly those specified in the manuscript.","The calculation does not assert zero bath-energy change or device implementation."],"dependencies":[{"kind":"claim","id":"C2","record_id":"RO-2026-0007"}],"evidence":[],"novelty_status":"apparently_new","review_status":"passed","reproduction_status":"passed","falsification_tests":["Recompute the full work histogram and Pearson values before and after the specified dephasing map."]},{"id":"C6","type":"computational_result","headline":false,"lifecycle":"established","statement":"Reduced equilibrium probes in the specified separable probe-ancilla model exhibit the fixed-score readout penalty without a drive or entangled source.","assumptions":["Only the probe marginals reach the detector.","Two distinct finite temperatures and the specified coupling are compared; no local-thermometry Fisher advantage is claimed."],"dependencies":[{"kind":"claim","id":"C3","record_id":"RO-2026-0007"}],"evidence":[],"novelty_status":"apparently_new","review_status":"passed","reproduction_status":"passed","falsification_tests":["Recompute the marked point's matrices and variance hierarchy at high precision."]},{"id":"C7","type":"corollary","headline":false,"lifecycle":"established","statement":"With characterized input states and calibrated outcome probabilities, a Pearson value above the product limit certifies an NPT readout effect in the stated copy partition.","assumptions":["The product hypotheses and partition used by C1 are fixed.","Input and measurement probabilities are characterized rather than inferred from two means alone."],"dependencies":[{"kind":"claim","id":"C1","record_id":"RO-2026-0007"}],"evidence":[],"novelty_status":"apparently_new","review_status":"passed","reproduction_status":"passed","falsification_tests":["Find a fully-PPT detector above the certified product threshold under the same calibration assumptions."]}],"literature_audit":{"protocol_version":"0.2.0","record_id":"RO-2026-0007","candidate_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","accepted_claims":["C1","C2","C3","C4","C5","C6","C7"],"search_cutoff":"2026-09-29","auditor":"Independent Pudim Physics Ledger Librarian, 2026-09-29","sources":["https://doi.org/10.1063/1.4905843","https://doi.org/10.1109/TIT.2025.3571527","https://doi.org/10.5281/zenodo.22069572","https://arxiv.org/html/2609.27767","https://doi.org/10.1088/0305-4470/38/7/014","https://doi.org/10.1103/PhysRevLett.130.260801","https://doi.org/10.1016/j.aop.2003.12.012","https://doi.org/10.1103/PhysRevA.72.042108","https://doi.org/10.1063/1.2168122","https://doi.org/10.1103/PhysRevA.80.052303","https://doi.org/10.1103/PhysRevE.75.050102","https://doi.org/10.1038/s41534-019-0138-y","https://doi.org/10.1103/PhysRevResearch.5.043184","https://doi.org/10.1103/PhysRevLett.107.050502","https://pudimphysics.org/research/RO-2026-0003","https://api.datacite.org/dois/10.5281/zenodo.22069572"],"queries":["fully PPT measured chi squared divergence tensorization product states measurement","PPT measured Renyi alpha 2 product states tensorization","separable measured chi-squared divergence product states","positive partial transpose Pearson quantum divergence","measured chi-squared superadditive noncommuting two copies","measured Renyi-2 noncommuting two copy strict","Two-Copy Onset Strict Superadditivity Measured Relative Entropy f-divergences","quadratic chi squared projective landscape commutator tensor product","fully PPT unbiased readout fixed observable added variance","quantum Hammersley Chapman Robbins restricted measurement variance","local global informationally complete measurement variance fixed bipartite observable","partial transpose POVM second moment variance observable","PPT measurement noise operator Schwarz fixed observable","partial transpose matrices of moments detector effects","post-drive energy dephasing leaves two point work distribution unchanged","quantum coherence work distribution dephasing after drive","collective readout Pearson gain dephasing thermodynamics","Ullah Naseem Mustecaplioglu reduced Gibbs probe coherence ancilla thermometry","reduced equilibrium probe fully PPT collective readout variance","temperature dependent reduced probe noncommuting two temperatures joint measurement","certify entangled measurement effect from distinguishability above PPT bound","device independent certification entangled measurements","PPT measurement witness calibrated input states Pearson divergence","Rippchen Sreekumar Berta PPT A1 through An B1 through Bn versus physical-copy partial transpose"],"inclusions":[{"citation":"K. Temme and F. Verstraete, Quantum chi-squared and goodness of fit testing, J. Math. Phys. 56, 012202 (2015), DOI 10.1063/1.4905843","identifier":"DOI:10.1063/1.4905843","url":"https://doi.org/10.1063/1.4905843","verified":true},{"citation":"T. Rippchen, S. Sreekumar and M. Berta, Locally-Measured Rényi Divergences, IEEE Trans. Inf. Theory 71(8), 6105–6133 (2025), DOI 10.1109/TIT.2025.3571527","identifier":"DOI:10.1109/TIT.2025.3571527","url":"https://doi.org/10.1109/TIT.2025.3571527","verified":true},{"citation":"Maestro v0.1, Two-Copy Onset of Strict Superadditivity for Measured Relative Entropy, Pudim AI Research Object RO-2026-0003 v1.0 (2026-08-23), DOI 10.5281/zenodo.22069572","identifier":"DOI:10.5281/zenodo.22069572","url":"https://doi.org/10.5281/zenodo.22069572","verified":true},{"citation":"D. S. P. Salazar, Benign Projective Landscapes for Measured Quantum Divergences, arXiv:2609.27767v1 (2026)","identifier":"arXiv:2609.27767v1","url":"https://arxiv.org/html/2609.27767","verified":true},{"citation":"Y. Tsuda and K. Matsumoto, Quantum estimation for non-differentiable models, J. Phys. A 38, 1593–1613 (2005), DOI 10.1088/0305-4470/38/7/014","identifier":"DOI:10.1088/0305-4470/38/7/014","url":"https://doi.org/10.1088/0305-4470/38/7/014","verified":true},{"citation":"M. Gessner and A. Smerzi, Hierarchies of Frequentist Bounds for Quantum Metrology: From Cramér–Rao to Barankin, Phys. Rev. Lett. 130, 260801 (2023), DOI 10.1103/PhysRevLett.130.260801","identifier":"DOI:10.1103/PhysRevLett.130.260801","url":"https://doi.org/10.1103/PhysRevLett.130.260801","verified":true},{"citation":"M. Ozawa, Uncertainty relations for noise and disturbance in generalized quantum measurements, Ann. Phys. 311, 350–416 (2004), DOI 10.1016/j.aop.2003.12.012","identifier":"DOI:10.1016/j.aop.2003.12.012","url":"https://doi.org/10.1016/j.aop.2003.12.012","verified":true},{"citation":"G. M. D’Ariano, P. Perinotti and M. F. Sacchi, Informationally complete measurements on bipartite quantum systems: Comparing local with global measurements, Phys. Rev. A 72, 042108 (2005), DOI 10.1103/PhysRevA.72.042108","identifier":"DOI:10.1103/PhysRevA.72.042108","url":"https://doi.org/10.1103/PhysRevA.72.042108","verified":true},{"citation":"G. M. D’Ariano, V. Giovannetti and P. Perinotti, Optimal estimation of quantum observables, J. Math. Phys. 47, 022102 (2006), DOI 10.1063/1.2168122","identifier":"DOI:10.1063/1.2168122","url":"https://doi.org/10.1063/1.2168122","verified":true},{"citation":"A. Miranowicz, M. Piani, P. Horodecki and R. Horodecki, Inseparability criteria based on matrices of moments, Phys. Rev. A 80, 052303 (2009), DOI 10.1103/PhysRevA.80.052303","identifier":"DOI:10.1103/PhysRevA.80.052303","url":"https://doi.org/10.1103/PhysRevA.80.052303","verified":true},{"citation":"P. Talkner, E. Lutz and P. Hänggi, Fluctuation theorems: Work is not an observable, Phys. Rev. E 75, 050102(R) (2007), DOI 10.1103/PhysRevE.75.050102","identifier":"DOI:10.1103/PhysRevE.75.050102","url":"https://doi.org/10.1103/PhysRevE.75.050102","verified":true},{"citation":"J. P. Santos, L. C. Céleri, G. T. Landi and M. Paternostro, The role of quantum coherence in non-equilibrium entropy production, npj Quantum Inf. 5, 23 (2019), DOI 10.1038/s41534-019-0138-y","identifier":"DOI:10.1038/s41534-019-0138-y","url":"https://doi.org/10.1038/s41534-019-0138-y","verified":true},{"citation":"A. Ullah, M. T. Naseem and Ö. E. Müstecaplıoğlu, Low-temperature quantum thermometry boosted by coherence generation, Phys. Rev. Research 5, 043184 (2023), DOI 10.1103/PhysRevResearch.5.043184","identifier":"DOI:10.1103/PhysRevResearch.5.043184","url":"https://doi.org/10.1103/PhysRevResearch.5.043184","verified":true},{"citation":"R. Rabelo, M. Ho, D. Cavalcanti, N. Brunner and V. Scarani, Device-independent certification of entangled measurements, Phys. Rev. Lett. 107, 050502 (2011), DOI 10.1103/PhysRevLett.107.050502","identifier":"DOI:10.1103/PhysRevLett.107.050502","url":"https://doi.org/10.1103/PhysRevLett.107.050502","verified":true}],"exclusions":[{"identifier":"DOI:10.1109/TIT.2025.3571527#special-family-additivity","reason":"General Lemma 4 establishes superadditivity for arbitrary IID pairs, not exact equality. Exact additive results for isotropic/Werner examples use a party A^n:B^n PPT cut, not PPT across every physical-copy subset for all faithful pairs; the article remains a verified nearest inclusion."},{"identifier":"DOI:10.5281/zenodo.22069572#relative-entropy-theorem","reason":"The two-copy noncommutation theorem is a genuine conceptual predecessor, but it uses measured relative entropy rather than the candidate measured Pearson objective; the record remains included."},{"identifier":"DOI:10.1103/PhysRevResearch.5.043184#probe-model","reason":"The reduced equilibrium probe model and its coherence are inherited, while the candidate C6 claim concerns a different finite-temperature fixed-score PPT readout comparison; the article remains included."}],"claim_assessments":[{"claim_id":"C1","closest_work":[{"citation":"Temme and Verstraete, Quantum chi-squared and goodness of fit testing, J. Math. Phys. 56, 012202 (2015).","identifier":"DOI:10.1063/1.4905843; arXiv:1112.6343","url":"https://doi.org/10.1063/1.4905843","verified":true},{"citation":"Rippchen, Sreekumar and Berta, Locally-Measured Renyi Divergences, IEEE Trans. Inf. Theory 71, 6105-6133 (2025).","identifier":"DOI:10.1109/TIT.2025.3571527; arXiv:2405.05037","url":"https://doi.org/10.1109/TIT.2025.3571527","verified":true}],"delta":"No equivalent result was identified under NL-3 as of 2026-09-29. Registered C1 has exact Q_N^fullyPPT = Q_1^N for faithful finite-dimensional IID pairs with physical-copy PPT cuts and local-score attainment. The Letter proves a broader unequal-copy product extension, also compared here, but it is not separately registered in claims.yaml.","unresolved_equivalences":["An older cone-duality or tensor cross-norm theorem under different terminology may imply the same fully-PPT IID equality or the broader Letter extension.","A specialist should check whether a non-obvious specialization of Rippchen et al. finite-order PPT variational upper bounds yields equality here."],"confidence":"MEDIUM","outcome":"PASS"},{"claim_id":"C2","closest_work":[{"citation":"Maestro v0.1, Two-Copy Onset of Strict Superadditivity for Measured Relative Entropy, Pudim AI RO-2026-0003 v1.0 (2026-08-23).","identifier":"DOI:10.5281/zenodo.22069572","url":"https://doi.org/10.5281/zenodo.22069572","verified":true},{"citation":"Salazar, Benign Projective Landscapes for Measured Quantum Divergences (2026).","identifier":"arXiv:2609.27767v1","url":"https://arxiv.org/html/2609.27767","verified":true},{"citation":"Rippchen, Sreekumar and Berta, Locally-Measured Renyi Divergences, IEEE Trans. Inf. Theory 71, 6105-6133 (2025).","identifier":"DOI:10.1109/TIT.2025.3571527; arXiv:2405.05037","url":"https://doi.org/10.1109/TIT.2025.3571527","verified":true}],"delta":"No explicit universal strict two-copy measured-Pearson criterion or positive ordered-commutator surplus formula was identified under NL-3 as of 2026-09-29. Credit is objective-specific; the general two-copy collective-gain phenomenon and relative-entropy analogue are prior.","unresolved_equivalences":["The strictness criterion may be an unstated corollary of earlier general optimizer calculus applied to the tensor-product score; method priority is less secure than explicit-result priority."],"confidence":"MEDIUM","outcome":"PASS"},{"claim_id":"C3","closest_work":[{"citation":"Ozawa, Uncertainty relations for noise and disturbance in generalized quantum measurements, Ann. Phys. 311, 350-416 (2004).","identifier":"DOI:10.1016/j.aop.2003.12.012; arXiv:quant-ph/0307057","url":"https://doi.org/10.1016/j.aop.2003.12.012","verified":true},{"citation":"D'Ariano, Perinotti and Sacchi, Informationally complete measurements on bipartite quantum systems: Comparing local with global measurements, Phys. Rev. A 72, 042108 (2005).","identifier":"DOI:10.1103/PhysRevA.72.042108; arXiv:quant-ph/0507104","url":"https://doi.org/10.1103/PhysRevA.72.042108","verified":true},{"citation":"Gessner and Smerzi, Hierarchies of Frequentist Bounds for Quantum Metrology, Phys. Rev. Lett. 130, 260801 (2023).","identifier":"DOI:10.1103/PhysRevLett.130.260801; arXiv:2303.06108","url":"https://doi.org/10.1103/PhysRevLett.130.260801","verified":true}],"delta":"No equivalent state-calibrated fixed-score fully-PPT positive added-variance statement was identified under NL-3 as of 2026-09-29. This theoretical witness depends on C1-C2 plus known POVM variance decomposition; it is not an implemented receiver, an exact PPT minimum, or independent novelty in quantum measurement noise.","unresolved_equivalences":["Earlier separable or PPT finite-displacement estimation theory may imply the same inequality without the candidate terminology."],"confidence":"MEDIUM","outcome":"PASS"},{"claim_id":"C4","closest_work":[{"citation":"Ozawa, Uncertainty relations for noise and disturbance in generalized quantum measurements, Ann. Phys. 311, 350-416 (2004).","identifier":"DOI:10.1016/j.aop.2003.12.012; arXiv:quant-ph/0307057","url":"https://doi.org/10.1016/j.aop.2003.12.012","verified":true},{"citation":"Miranowicz, Piani, Horodecki and Horodecki, Inseparability criteria based on matrices of moments, Phys. Rev. A 80, 052303 (2009).","identifier":"DOI:10.1103/PhysRevA.80.052303; arXiv:quant-ph/0605001","url":"https://doi.org/10.1103/PhysRevA.80.052303","verified":true}],"delta":"A scoped detector-effect moment refinement for prescribed-operator readout was not found explicitly under NL-3 as of 2026-09-29. It is only a necessary lower bound and carries limited independent conceptual novelty.","unresolved_equivalences":["The short cutwise Schwarz step could be implicit in older positive-map measurement theory under other terminology."],"confidence":"LOW","outcome":"PASS"},{"claim_id":"C5","closest_work":[{"citation":"Talkner, Lutz and Hänggi, Fluctuation theorems: Work is not an observable, Phys. Rev. E 75, 050102(R) (2007).","identifier":"DOI:10.1103/PhysRevE.75.050102; arXiv:cond-mat/0703189","url":"https://doi.org/10.1103/PhysRevE.75.050102","verified":true},{"citation":"Maestro v0.1, Two-Copy Onset of Strict Superadditivity for Measured Relative Entropy, Pudim AI RO-2026-0003 v1.0 (2026-08-23).","identifier":"DOI:10.5281/zenodo.22069572","url":"https://doi.org/10.5281/zenodo.22069572","verified":true},{"citation":"Santos, Céleri, Landi and Paternostro, The role of quantum coherence in non-equilibrium entropy production, npj Quantum Inf. 5, 23 (2019).","identifier":"DOI:10.1038/s41534-019-0138-y; arXiv:1707.08946","url":"https://doi.org/10.1038/s41534-019-0138-y","verified":true}],"delta":"The four-spin model calculation and its scoped comparison of disappearing Pearson readout surplus with unchanged full two-point work histogram appear candidate-specific. No credit is assigned to the general dephasing or work-statistics mechanism.","unresolved_equivalences":["No exhaustive search of every driven-medium numerical parameterization was performed.","This is an ideal-model computation, not a detector implementation, energetic-cost result, or exact restricted variance optimum."],"confidence":"LOW","outcome":"PASS"},{"claim_id":"C6","closest_work":[{"citation":"Ullah, Naseem and Müstecaplıoğlu, Low-temperature quantum thermometry boosted by coherence generation, Phys. Rev. Research 5, 043184 (2023).","identifier":"DOI:10.1103/PhysRevResearch.5.043184; arXiv:2211.05461","url":"https://doi.org/10.1103/PhysRevResearch.5.043184","verified":true}],"delta":"The fixed-score fully-PPT variance hierarchy evaluated on the imported reduced-equilibrium model appears candidate-specific. Neither the Hamiltonian nor coherence-enhanced local thermometry is new here.","unresolved_equivalences":["Follow-up papers using the same probe model were not exhaustively checked for identical parameter points or readout observables.","The plotted hierarchy is an ideal-model calculation without hardware or local-Fisher advantage."],"confidence":"LOW","outcome":"PASS"},{"claim_id":"C7","closest_work":[{"citation":"Rabelo, Ho, Cavalcanti, Brunner and Scarani, Device-independent certification of entangled measurements, Phys. Rev. Lett. 107, 050502 (2011).","identifier":"DOI:10.1103/PhysRevLett.107.050502; arXiv:1105.3138","url":"https://doi.org/10.1103/PhysRevLett.107.050502","verified":true},{"citation":"Rippchen, Sreekumar and Berta, Locally-Measured Renyi Divergences, IEEE Trans. Inf. Theory 71, 6105-6133 (2025).","identifier":"DOI:10.1109/TIT.2025.3571527; arXiv:2405.05037","url":"https://doi.org/10.1109/TIT.2025.3571527","verified":true}],"delta":"The calibrated population bound Q_n > Q_1^n excludes every fully-PPT POVM and implies at least one NPT effect by C1. Full outcome probabilities and a characterized input pair are required. This is a dependent theoretical corollary, not independent priority for entangled-measurement certification or a finite-shot detector demonstration.","unresolved_equivalences":["Other restricted-measurement witnesses may admit an equivalent Pearson rephrasing."],"confidence":"LOW","outcome":"PASS"}],"overall_outcome":"PASS"},"review":{"protocol_version":"0.2.0","record_id":"RO-2026-0007","accepted_claims":["C1","C2","C3","C4","C5","C6","C7"],"rounds":[{"round":1,"candidate_digest":"5628b603233c435844a718fc94b8895a57a1491e636431aa9775fa5aa7fdf52e","opened_at":"2026-09-29T20:24:23Z","closed_at":"2026-09-29T20:34:07Z","referees":[{"id":"R1","context_isolated":true,"report_path":"reviews/round-01/reviewer1.md","recommendation":"MAJOR_REVISION","confidence":0.78,"verification_scope":"Theorem algebra, novelty, physical interpretation, and fixed-score significance."},{"id":"R2","context_isolated":true,"report_path":"reviews/round-01/reviewer2.md","recommendation":"MAJOR_REVISION","confidence":0.88,"verification_scope":"Evidence, source hashes, marked-point arithmetic, finite-shot calibration, and presentation."}],"editor":{"independent_context":true,"decision":"MAJOR_REVISION","confidence":0.79,"letter_path":"reviews/round-01/editor.md","decisive_evidence":["Both referees found C1-C4 and C7 mathematically credible.","The physical interpretation, fixed-operator bracket, nearest-work distinction, and finite-shot caution needed revision."]},"findings":[{"id":"F-R1-001","criterion":"physical-interpretation","severity":"major","affected_claims":["C3","C5","C6"],"finding":"State-calibrated collective score lacked a clear independent readout purpose.","evidence":["reviews/round-01/reviewer1.md","reviews/round-01/editor.md"],"response":"v033 frames the score as a theoretical witness and narrows the model interpretation.","resolution":"resolved"},{"id":"F-R1-002","criterion":"fixed-operator-scope","severity":"major","affected_claims":["C3","C4","C6"],"finding":"The exact prescribed-score PPT minimum and feasible receiver gap were not adjacent to application claims.","evidence":["reviews/round-01/reviewer1.md","reviews/round-01/reviewer2.md"],"response":"v033 states the unknown minimum and marked-point lower/upper bracket beside Fig. 2.","resolution":"resolved"},{"id":"F-R1-003","criterion":"prior-work-attribution","severity":"major","affected_claims":["C1","C2"],"finding":"Closest restricted-Renyi work needed objective, product-input, and cut comparison.","evidence":["reviews/round-01/reviewer1.md","reviews/round-01/editor.md"],"response":"v033 scoped the comparison; v034 names general superadditivity and special exact-additivity examples precisely.","resolution":"resolved"},{"id":"F-R1-004","criterion":"finite-shot-calibration","severity":"major","affected_claims":["C6","C7"],"finding":"The rare product-receiver outcome made a population curve inadequate as a finite-shot certificate.","evidence":["reviews/round-01/reviewer2.md"],"response":"v033 quantifies the missed-outcome probability and makes no receiver validation or shot-budget claim.","resolution":"resolved"},{"id":"F-R1-005","criterion":"external-APS-policy","severity":"note","affected_claims":[],"finding":"AI author byline and disclosure would require a different actual APS process.","evidence":["reviews/round-01/reviewer2.md","reviews/round-01/editor.md"],"response":"Pudim credit follows the PM direction; no APS submission is claimed.","resolution":"accepted"}],"author_response":{"actor":"Codex 5.6 Sol","path":"reviews/round-01/author-response-v033.md","submitted_at":"2026-09-29T20:42:57Z"},"revision_digest":"4e03aa9526b3547fd33043fe4c507dea9e5b37548a0ab22c15f1c737bce4d401","outcome":"INCONCLUSIVE"},{"round":2,"candidate_digest":"4e03aa9526b3547fd33043fe4c507dea9e5b37548a0ab22c15f1c737bce4d401","opened_at":"2026-09-29T20:47:17Z","closed_at":"2026-09-29T21:07:45Z","referees":[{"id":"R1","context_isolated":true,"report_path":"reviews/round-02/reviewer1.md","recommendation":"MINOR_REVISION","confidence":0.77,"verification_scope":"Complete Letter and supplement, own prior findings, theorem, marked-point independent matrix check."},{"id":"R2","context_isolated":true,"report_path":"reviews/round-02/reviewer2.md","recommendation":"MINOR_REVISION","confidence":0.88,"verification_scope":"Complete Letter and supplement, manifest, marked-point independent computation, figures and claim scope."}],"editor":{"independent_context":true,"decision":"ACCEPT","confidence":0.84,"letter_path":"reviews/round-02/editor-v034-addendum.md","decisive_evidence":["Both independent referees voted PRL scientific threshold YES and Pudim adversarial PASS on v033.","The independent editor requested only a nearest-work precision edit and a small focus trim.","Exact-digest v034 editor addendum verifies both requests and no loss of caveats.","Independent Solver, Breaker, and Librarian rebind v034 with no changed scientific claim."]},"findings":[{"id":"F-R2-001","criterion":"nearest-work-precision","severity":"minor","affected_claims":["C1","C2"],"finding":"The Rippchen sentence compressed a general result into its special-family examples.","evidence":["reviews/round-02/reviewer1.md","reviews/round-02/reviewer2.md","reviews/round-02/editor.md"],"response":"v034 explicitly states general superadditivity and special-family exact-additivity under grouped-party cuts.","resolution":"resolved"},{"id":"F-R2-002","criterion":"letter-focus","severity":"minor","affected_claims":["C5","C6"],"finding":"The second model repeated receiver and bound descriptions in a four-page Letter.","evidence":["reviews/round-02/reviewer1.md","reviews/round-02/editor.md"],"response":"v034 trims repeated prose, keeping both figures, numerical bracket and all limitations; exact-digest editor approved.","resolution":"resolved"},{"id":"F-R2-003","criterion":"external-APS-policy","severity":"note","affected_claims":[],"finding":"Actual APS submission requires separate compliant authorship, AI-use disclosure and data availability.","evidence":["reviews/round-02/reviewer2.md","reviews/round-02/editor.md"],"response":"This is a Pudim Ledger candidate and no APS submission is claimed.","resolution":"accepted"}],"author_response":{"actor":"Codex 5.6 Sol","path":"reviews/round-02/author-response-v034.md","submitted_at":"2026-09-29T21:05:20Z"},"revision_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","outcome":"PASS"}],"ledger_decision":{"decision":"GO","candidate_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","authority":"Independent Pudim Physics Ledger scientific editor","decided_at":"2026-09-29T21:33:58Z","rationale":"Exact-digest v034 editorial GO follows successful blind and computational reproduction, both context-isolated review rounds, and resolution of all scientific findings; release still requires separate Program Manager authorization."}},"replication":{"protocol_version":"0.2.0","record_id":"RO-2026-0007","replicator":"Independent RO-2026-0007 Replicator, 2026-09-29","independent_of":["solver","reviewer","publisher"],"started_at":"2026-09-29T21:14:10Z","completed_at":"2026-09-29T21:26:46Z","claim_results":[{"claim_id":"C1","mode":"theoretical","blinded_to_solver_proof_initially":true,"inputs":["runs/20260929T210823Z/REPRODUCTION/inputs/replication/initial-theorem-packet.md","runs/20260929T211408Z/REPRODUCTION/inputs/paper/candidate-v1.0.zip","runs/20260929T211408Z/REPRODUCTION/inputs/proofs/solver-20260929/report.md","runs/20260929T211408Z/REPRODUCTION/inputs/proofs/solver-20260929/v034-rebind/report.md"],"artifacts":["replication/blind-v034/attempt.md","replication/v034-final/report.md","replication/v034-final/spotcheck.json"],"comparison":"Independent cutwise Cauchy-Schwarz proof matches the manuscript positive-square decomposition term by term and proves the unequal-register full-PPT upper bound; the product of local score PVMs attains it. Exact final archive digest 3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0 and all 108 payload hashes verified.","outcome":"PASS"},{"claim_id":"C2","mode":"theoretical","blinded_to_solver_proof_initially":true,"inputs":["runs/20260929T210823Z/REPRODUCTION/inputs/replication/initial-theorem-packet.md","runs/20260929T211408Z/REPRODUCTION/inputs/paper/candidate-v1.0.zip","runs/20260929T211408Z/REPRODUCTION/inputs/proofs/solver-20260929/report.md"],"artifacts":["replication/blind-v034/attempt.md","replication/v034-final/report.md"],"comparison":"Blind Jordan residual and positive inverse-Jordan quadratic agree with supplement.tex 148-171 and Solver C2. Surplus is strictly positive exactly when both local pairs fail to commute; it vanishes if either pair commutes.","outcome":"PASS"},{"claim_id":"C3","mode":"theoretical","blinded_to_solver_proof_initially":true,"inputs":["runs/20260929T210823Z/REPRODUCTION/inputs/replication/initial-theorem-packet.md","runs/20260929T211408Z/REPRODUCTION/inputs/paper/candidate-v1.0.zip","runs/20260929T211408Z/REPRODUCTION/inputs/proofs/solver-20260929/report.md"],"artifacts":["replication/blind-v034/attempt.md","replication/v034-final/report.md"],"comparison":"Independent normalization, classical Pearson Cauchy-Schwarz, and C1 give intrinsic variance 1/(Q_n-1) and the necessary fixed-score added variance 1/(Q_1^n-1)-1/(Q_n-1). Manuscript and Solver steps agree. No fixed-score restricted-minimum attainment is inferred.","outcome":"PASS"},{"claim_id":"C4","mode":"theoretical","blinded_to_solver_proof_initially":true,"inputs":["runs/20260929T210823Z/REPRODUCTION/inputs/replication/initial-theorem-packet.md","runs/20260929T211408Z/REPRODUCTION/inputs/paper/candidate-v1.0.zip","runs/20260929T211408Z/REPRODUCTION/inputs/proofs/solver-20260929/report.md"],"artifacts":["replication/blind-v034/attempt.md","replication/v034-final/report.md","replication/v034-final/spotcheck.json"],"comparison":"Blind attempt independently proved the cutwise transposed-POVM moment floor. It did not prove the manuscript's stronger second-line hierarchy. Phase-two audit separately verified the cut average equals the product-Jordan quadratic form and Cauchy-Schwarz gives b_mom at least j(A)^2/(product Q_j-1). Marked-point average 34.76681194676327 lies between moment floor 49.51983479130428 and class-wide floor 20.279850633410486.","outcome":"PASS"},{"claim_id":"C5","mode":"computational","blinded_to_solver_proof_initially":true,"inputs":["runs/20260929T211408Z/REPRODUCTION/inputs/paper/candidate-v1.0.zip","replication/pc2-numerical/canonical-import-receipt.json","replication/pc2-numerical/completion-receipt.json","reproduction/v1.0/attestation/run.json","reproduction/v1.0/attestation/tier2.json"],"artifacts":["replication/v034-final/report.md","replication/v034-final/spotcheck.py","replication/v034-final/spotcheck.json"],"environment":"Earlier PC2 Windows fresh-environment rerun; exact-candidate offline rootless non-root Linux Podman tiers on PC1; independent local NumPy read-only spot check. Podman execution isolation was attested, not personally witnessed by this replicator.","commands":["python replication/v034-final/spotcheck.py runs/20260929T211408Z/REPRODUCTION .","reconstruction/reproduce.py --tier 0/1/2 via attested rootless Podman runner"],"tolerances":["Thermal CSV 251 rows, rtol 1e-7 and atol 1e-9; observed attested max absolute difference 4.27e-14.","Independent full 256-transition work histogram maximum difference 5.55e-17.","Independent four-delay quartic-law maximum residual 4.88e-15."],"comparison":"PC2 ran 10 successful scripts against the earlier f5df5a archive; all 98 code/data/figure members are byte identical to final v034. Exact-final Linux tier 0/1/2 hashes and zero exits verified. Independent formulas recover Q1 4.976657014386025, Q2 29.41658405300647, positive initial surplus 4.649469014168844, numerical zero after complete dephasing, unchanged full TPM distribution, and initial moment floor 0.15485916898364083. This is model reproduction, not a device or heat-cost experiment.","outcome":"PASS"},{"claim_id":"C6","mode":"computational","blinded_to_solver_proof_initially":true,"inputs":["runs/20260929T211408Z/REPRODUCTION/inputs/paper/candidate-v1.0.zip","replication/pc2-numerical/canonical-import-receipt.json","reproduction/v1.0/attestation/run.json","reproduction/v1.0/attestation/tier2.json"],"artifacts":["replication/v034-final/report.md","replication/v034-final/spotcheck.py","replication/v034-final/spotcheck.json"],"environment":"Exact-candidate offline rootless non-root Linux Podman tiers plus independent local NumPy evaluation of archived states and the 36-effect product POVM.","commands":["python replication/v034-final/spotcheck.py runs/20260929T211408Z/REPRODUCTION .","reconstruction/reproduce.py --tier 0/1/2 via attested rootless Podman runner"],"tolerances":["Equilibrium CSV 196 rows, rtol 1e-7 and atol 1e-9; observed attested max absolute difference 2.26e-11.","Marked NPZ 13 arrays, rtol 1e-7 and atol 1e-9; observed attested max absolute difference 1.71e-12.","Independent product first-moment residual 4.00e-10 against separately recomputed Astar."],"comparison":"The reduced Gibbs marginal formula, noncommuting probe states, joint Jordan score, cut moments, full-Gibbs commutation, and feasible product POVM were independently checked. Marked intrinsic/class/moment/product variances are 20.01378910222163, 20.279850633410486, 49.51983479130428, and 195.8199527967509. No local Fisher advantage, exact PPT minimum, or experiment is inferred.","outcome":"PASS"},{"claim_id":"C7","mode":"theoretical","blinded_to_solver_proof_initially":true,"inputs":["runs/20260929T210823Z/REPRODUCTION/inputs/replication/initial-theorem-packet.md","runs/20260929T211408Z/REPRODUCTION/inputs/paper/candidate-v1.0.zip","runs/20260929T211408Z/REPRODUCTION/inputs/proofs/solver-20260929/report.md"],"artifacts":["replication/blind-v034/attempt.md","replication/v034-final/report.md"],"comparison":"The blind contrapositive of C1 agrees with final manuscript and Solver: exceeding the product Pearson threshold under characterized product inputs and calibrated full outcome laws forces at least one effect to fail PPT on a physical-register cut. No converse or finite-shot claim.","outcome":"PASS"}],"overall_outcome":"PASS"},"reproduction":{"protocol_version":"0.2.0","record_id":"RO-2026-0007","candidate_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","accepted_claims":["C1","C2","C3","C4","C5","C6","C7"],"entrypoint":"reconstruction/reproduce.py","container":{"image":"pudim-ro-2026-0007:v1.0","digest":"sha256:cc6dbfdd040582433b5f7e698206a9ae612dfd0d19d178d7563ae87f8b654acb","lockfiles":["reconstruction/Containerfile","reconstruction/requirements-lock.txt","reconstruction/reproduce.py","paper/source/MANIFEST.json"]},"offline":true,"non_root":true,"reference_runner":{"os":"linux","vcpus":8,"memory_gb":8},"tiers":[{"tier":0,"description":"Verify final archive SHA-256, all 108 manifest members and ZIP CRC, without network or writable root.","maximum_seconds":120,"commands":["podman run --rm --network none --read-only --tmpfs /tmp:rw,size=2g,mode=1777 --user 65532:65532 --cpus 8 --memory 8g --cap-drop all --security-opt no-new-privileges -e HOME=/tmp -e MPLCONFIGDIR=/tmp/mpl pudim-ro-2026-0007:v1.0 --tier 0"],"outcome":"PASS"},{"tier":1,"description":"Run six independent code-level algebra, moment, thermal, equilibrium and seeded-simulation validators.","maximum_seconds":300,"commands":["podman run --rm --network none --read-only --tmpfs /tmp:rw,size=2g,mode=1777 --user 65532:65532 --cpus 8 --memory 8g --cap-drop all --security-opt no-new-privileges -e HOME=/tmp -e MPLCONFIGDIR=/tmp/mpl pudim-ro-2026-0007:v1.0 --tier 1"],"outcome":"PASS"},{"tier":2,"description":"Regenerate the driven and equilibrium numeric scans, marked matrices, seeded count data and both main figures; compare declared numeric tolerances.","maximum_seconds":600,"commands":["podman run --rm --network none --read-only --tmpfs /tmp:rw,size=2g,mode=1777 --user 65532:65532 --cpus 8 --memory 8g --cap-drop all --security-opt no-new-privileges -e HOME=/tmp -e MPLCONFIGDIR=/tmp/mpl pudim-ro-2026-0007:v1.0 --tier 2"],"outcome":"PASS"}],"expected_outputs":[{"path":"reproduction/v1.0/attestation/tier0.json","kind":"data","comparison":"hash","expected_sha256":"5173e0bf84ff17d9412faee96d6c8d1a44e4459176bb501c3d4bfd01657cb1d5"},{"path":"reproduction/v1.0/attestation/tier1.json","kind":"data","comparison":"hash","expected_sha256":"ac6c3e3a74bf624f846c434e1871747746bc87af1d43b481c58bd3f2714448a6"},{"path":"reproduction/v1.0/attestation/tier2.json","kind":"data","comparison":"hash","expected_sha256":"26214b4b6ba000b03c24a2b21b772423057c8c33d95804e378727a05bc52b848"}],"scientific_tolerances":[{"output":"data/thermo_moment_bounds.csv","metric":"all numeric cells after independent regeneration","tolerance":"rtol 1e-7, atol 1e-9; observed max absolute difference 4.27e-14"},{"output":"data/equilibrium_readout_scan.csv","metric":"all numeric cells after independent regeneration","tolerance":"rtol 1e-7, atol 1e-9; observed max absolute difference 2.26e-11"},{"output":"data/equilibrium_marked_matrices.npz","metric":"all 13 array members after independent regeneration","tolerance":"rtol 1e-7, atol 1e-9; observed max absolute difference 1.71e-12"},{"output":"figures/fig1_thermal_moments.pdf and figures/fig2_equilibrium_moments.pdf","metric":"regeneration from numeric data","tolerance":"files exist and render; PDF byte identity not required across Matplotlib versions"}],"attestation":{"run_path":"reproduction/v1.0/attestation/run.json","image_digest":"sha256:cc6dbfdd040582433b5f7e698206a9ae612dfd0d19d178d7563ae87f8b654acb","lock_hashes":{"reconstruction/Containerfile":"87a95074d6c117944dc30a31c17f2c35a5033ab504216c4e535c2817006604a6","reconstruction/requirements-lock.txt":"b7d59aabc9b78a1c3d04f72b6b2586002242877a41b5935e7ab81aa40b0c28c7","reconstruction/reproduce.py":"f1c7d87e59e68c964bdd82d6139d86766f181584f9102c1be8d3605837d26af6","paper/source/MANIFEST.json":"0944fb60597851dd616d901177a41a85d723b1f5209c37e68195a1be13f022d1"},"started_at":"2026-09-29T21:11:32.386862Z","completed_at":"2026-09-29T21:12:02.958996Z","resources":{"runner":"rootless Podman under WSL2 Ubuntu on PC1","vcpus_ceiling":8,"memory_gb_ceiling":8,"uid":65532,"network":"none","root_filesystem":"read-only","capabilities":"all dropped; no-new-privileges","tmpfs":"/tmp 2 GiB","pc2_reason":"Earlier fresh-environment numerical rerun on PC2 completed and imported; OCI runner requires Linux Podman available on PC1 WSL, not PC2 Windows."},"exit_codes":{"tier_0":0,"tier_1":0,"tier_2":0},"output_hashes":{"reproduction/v1.0/attestation/tier0.json":"5173e0bf84ff17d9412faee96d6c8d1a44e4459176bb501c3d4bfd01657cb1d5","reproduction/v1.0/attestation/tier0.jsonlog":"85a8528f75dc3e10c086ca7762e2a0c190f89d471eec87de50ef7b8b83109555","reproduction/v1.0/attestation/tier1.json":"ac6c3e3a74bf624f846c434e1871747746bc87af1d43b481c58bd3f2714448a6","reproduction/v1.0/attestation/tier1.jsonlog":"07e08f795b3e13d1697aa21a5b4e59dc43dc27a61ecb0877739fd2b8c73bc744","reproduction/v1.0/attestation/tier2.json":"26214b4b6ba000b03c24a2b21b772423057c8c33d95804e378727a05bc52b848","reproduction/v1.0/attestation/tier2.jsonlog":"a68be165ceebba7512f01bc34886c12e6475b87b1260ae8bd8adffb3896a63cc"},"gate_results":[{"id":"tier_0","outcome":"PASS"},{"id":"tier_1","outcome":"PASS"},{"id":"tier_2","outcome":"PASS"}]},"overall_outcome":"PASS"},"editorial_decision":{"protocol_version":"0.2.0","record_id":"RO-2026-0007","candidate_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","ledger_decision":{"decision":"GO","authority":"Independent Pudim Physics Ledger scientific editor","decided_at":"2026-09-29T21:33:58Z","rationale":"Exact-digest packet integrity, scoped claims C1-C7, candidate-bound novelty, two-round adversarial review with final editorial and proof rebinds, blind theoretical reconstruction, final numerical spot checks, and attested offline container reproduction support scientific acceptance. No unresolved scientific blocker remains within the stated theoretical and ideal-model scope."},"pm_release_authorization":{"authorized":true,"name":"Domingos S. P. Salazar","role":"Program Manager","authorized_at":"2026-09-29T22:00:57Z","rationale":"In this task, the Program Manager answered \"Authorized\" to the explicit exact-digest request to release RO-2026-0007 v1.0, source SHA-256 3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0, at pudimphysics.org/research/RO-2026-0007 with a production Zenodo DOI. This authorization does not approve a future Correspondent Story digest."},"accepted_claims":["C1","C2","C3","C4","C5","C6","C7"],"evidence":["editorial/report-v1.0.md","runs/20260929T212926Z/EDITORIAL_DECISION/manifest.json","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/paper/candidate-v1.0.zip","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/claims.yaml","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/literature/librarian-20260929/literature-audit-v034.yaml","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/literature/librarian-20260929/v034-carry.md","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/reviews/review-v1.0.yaml","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/reviews/round-02/editor-v034-addendum.md","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/proofs/solver-20260929/v034-rebind/verdict.json","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/proofs/breaker-20260929/v034-rebind/verdict.json","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/replication/blind-v034/attempt.md","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/replication/v034-final/report.md","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/replication/replication-v1.0.yaml","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/reproduction/reproduction-v1.0.yaml","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/reproduction/v1.0/attestation/run.json","runs/20260929T212926Z/EDITORIAL_DECISION/inputs/provenance/provenance-v1.0.json"],"blocking_findings_disposition":["F-R1-001 through F-R1-004: resolved by the scoped v033 manuscript and exact-digest v034 carry.","F-R2-001 and F-R2-002: resolved in the exact v034 archive, as verified by the independent editor addendum.","F-R1-005 and F-R2-003: accepted external APS policy notes; no APS submission or acceptance is claimed.","No open correctness, novelty-gate, review, or reproduction blocker remains for the accepted scope."],"conditions":["Decision applies only to SHA-256 3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0.","C3 and C4 concern an operator-unbiased, state-calibrated fixed score; the exact fully-PPT minimum is unknown.","C5 and C6 are ideal finite-model calculations, not hardware or energetic-cost demonstrations; C5 zero surplus is the complete-dephasing limit.","C7 requires characterized inputs and calibrated full outcome laws and makes no finite-shot or device-independent claim.","Novelty confidence and unresolved equivalence questions must remain visible; global priority is not certified.","Scientific GO confers no release authority; a separate explicit Program Manager authorization bound to this digest is required."]},"provenance":{"protocol_version":"0.2.0","record_id":"RO-2026-0007","agents":[{"name":"Codex 5.6 Sol","role":"Requested scientific author credit","identifier":"codex-5.6-sol","version":"5.6","model":null,"model_snapshot":null,"provider":"OpenAI","model_knowledge_cutoff":null,"literature_cutoff":null}],"task_specifications":[],"tools":[{"name":"Pudim Physics Research Ledger","version":"0.2.0","scientific_purpose":"Archive intake, claim registry, frozen-stage packets, and release gates."},{"name":"MiKTeX REVTeX 4.2 and BibTeX","version":null,"scientific_purpose":"Rebuild the author-credit Letter and supplement."},{"name":"Python NumPy SciPy Matplotlib","version":null,"scientific_purpose":"Recompute deterministic example data and figures."},{"name":"Rootless Podman OCI reconstruction","version":"image sha256:cc6dbfdd040582433b5f7e698206a9ae612dfd0d19d178d7563ae87f8b654acb","scientific_purpose":"Offline exact-archive hash, proof-validator and numerical-regeneration tiers."}],"sources":[],"environments":["PC1 Windows, Python 3.11, MiKTeX REVTeX 4.2, Poppler","PC2 Windows, isolated Python environment for independent numerical rerun; all checks completed and imported","PC1 WSL2 Ubuntu rootless Podman, 8 vCPU/8 GiB constrained, network disabled, read-only root, uid 65532"],"datasets":["paper/source/data/thermo_moment_bounds.csv","paper/source/data/equilibrium_readout_scan.csv","paper/source/data/equilibrium_marked_matrices.npz","paper/source/data/monte_carlo/"],"random_seeds":["Recorded in deterministic simulation scripts and data files."],"material_artifacts":["claims.yaml","reconstruction/Containerfile","reconstruction/requirements-lock.txt","reconstruction/reproduce.py","reproduction/reproduction-v1.0.yaml","replication/replication-v1.0.yaml"],"disclosures":{"private_chain_of_thought_preserved":false,"secrets_included":false,"notes":["The v030 supplied manuscript named Domingos S. P. Salazar as author. The Program Manager instructed this v031 Ledger candidate to credit Codex 5.6 Sol instead and to record Domingos separately as Program Manager.","The available local history does not independently identify every model that contributed to prior drafts; model snapshot metadata is left unasserted. The requested byline is not an execution log.","v032 adds two explicit related-work attribution sentences and a bibliography DOI; theorem statements, equations, figures, code, and data remain unchanged.","v033 answers the first independent review round with more explicit theoretical-witness scope, a finite-shot caveat, and corrected readout-bound terminology; mathematical equations and numerical inputs are unchanged under independent digest-bound audits.","v034 applies the second-round editor requests to attribution and focus only; equations, numerical inputs, and figures are unchanged under digest-bound audits.","For v034, two independent PRL-style referees and a separate editor completed two rounds. A fresh-context blind Replicator then passed C1-C7, and an offline rootless Linux container regenerated the model data and figures within declared tolerances. Ledger editorial and release authority are separate decisions."]}},"release_manifest":{"protocol_version":"0.2.0","record_id":"RO-2026-0007","release":"v1.0","candidate_digest":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","accepted_claims":["C1","C2","C3","C4","C5","C6","C7"],"created_at":"2026-09-29T22:00:57.000Z","git_commit":"0583d9a86ec344388b9dd23965c089303018ed4c","build":{"builder":"research-ledger-publisher/0.2.0","reproducible":true,"source_date_epoch":1790719257},"files":[{"path":"citation.bbl","sha256":"9b3b149c558a0ff8f5477fe13b57c3d4b900ad14b9d02c0366ba071123d9381e","bytes":282,"media_type":"application/x-tex","license":"CC-BY-4.0"},{"path":"citation.bib","sha256":"d5f766e43b60fcbf375c2df9b4c9f4dd7e51bbbbd0e3ccf7ff4bf43c4c14a44c","bytes":1402,"media_type":"application/x-bibtex","license":"CC-BY-4.0"},{"path":"CITATION.cff","sha256":"1f3ab0c235a3736fa22ef09110be39dc10d9183be44d940b7b634ae6526ff641","bytes":1896,"media_type":"application/yaml","license":"CC-BY-4.0"},{"path":"citation.csl.json","sha256":"7cb00aa2d8cfe9f851047f89449b476aa7923d894c7489bfd6ec506743a685b8","bytes":1523,"media_type":"application/json","license":"CC-BY-4.0"},{"path":"claims.yaml","sha256":"a00bae1c5cbfd3440989ee942d918cdca24150f76d296c6abb8696d60f96c362","bytes":6911,"media_type":"application/yaml","license":"CC-BY-4.0"},{"path":"editorial/editorial-decision-v1.0.yaml","sha256":"61bfc24a84fb1efbc3c539a42c8e32091f83d0c9e1bebadeddd4d454bc5ccf1b","bytes":3822,"media_type":"application/yaml","license":"CC-BY-4.0"},{"path":"literature/librarian-20260929/literature-audit-v034.yaml","sha256":"16751945a0b25024d1bd7dbcb3b3835127dc160f601045bd3a7150de057ada7c","bytes":16396,"media_type":"application/yaml","license":"CC-BY-4.0"},{"path":"paper/public/article.pdf","sha256":"1d0c40881fbd473596855343fec8973c6212d15426f79f428e6e5b4fd19f496d","bytes":474701,"media_type":"application/pdf","license":"CC-BY-4.0"},{"path":"paper/public/candidate-v1.0.zip","sha256":"3c0cfd6bd6286def714daa4e3b833d62400f7baf61d9fb91fd796bb80b09a0b0","bytes":5273077,"media_type":"application/zip","license":"CC-BY-4.0"},{"path":"paper/public/combined.pdf","sha256":"a8407cfe50d98d6fd9f74f47026671c63c70ff21151a2991edd35d5ce25822f7","bytes":880642,"media_type":"application/pdf","license":"CC-BY-4.0"},{"path":"paper/public/README.md","sha256":"8cdbeae8c5e242f67b97381fd3868725e2f02ca475d1ff95aff0caea5335b8de","bytes":1048,"media_type":"text/markdown","license":"CC-BY-4.0"},{"path":"paper/public/supplement.pdf","sha256":"6a5d228a09b2bf8847f401dbd1e89d46f9db92b1c4ffe4acfebba264b41787f7","bytes":421357,"media_type":"application/pdf","license":"CC-BY-4.0"},{"path":"paper/source/data/binary_design.json","sha256":"813ad8942a562ae330e0d17b972d929506c32a46e0d17192c92bc658ab55eef8","bytes":2090,"media_type":"application/json","license":"CC-BY-4.0"},{"path":"paper/source/data/binary_detection_curve.csv","sha256":"dead75347cbde7152d9c562197419f9a8be11b1e92af5495290c0240f2b9530f","bytes":25082,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/collective_walk.csv","sha256":"b2fee996a06216995a4c04446b34e491df1b5420442f6b986fbe9ca9ba38aca4","bytes":300136,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/detection_exponent_example.json","sha256":"4a60759e3a14429f839dff7dbc759eab6bae36d89e585861361b0d4d19b905db","bytes":460,"media_type":"application/json","license":"CC-BY-4.0"},{"path":"paper/source/data/equilibrium_marked_matrices.npz","sha256":"252a6bdb4851e24235463d1faad832b212420b2fc3f03fc8bbd5733db6021220","bytes":4826,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/equilibrium_marked.json","sha256":"f699f638a86b7b0abf3610a47c990ed29484c6b9e674f0da5d79b097899dcff2","bytes":1210,"media_type":"application/json","license":"CC-BY-4.0"},{"path":"paper/source/data/equilibrium_readout_scan.csv","sha256":"a1d0ccd174eebbee9f6b83dbed0ea8a3df2dec5298a95dfc0cf72177ebc0504f","bytes":74451,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/finite_batching.csv","sha256":"0f506fb3cea15da735cd880d2a6f9c20a68c49e892b3615a3864de71d970b2ec","bytes":150046,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/fisher_batching.csv","sha256":"a2becef64f7138ca271daefc797b9853f82353e57d337b5505412aecbc74f803","bytes":3670,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_015_product.npz","sha256":"0bd99cc5208d367e81f4bbd208e1c602c1b2a6805a961dc93b3f66d2bc5ccda3","bytes":9018,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_015_spectral.npz","sha256":"41c24145240623954d22f2496c50df65869157b61d397ce07334944a8b17a388","bytes":4256,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_035_product.npz","sha256":"4493d9bb41ee71d50b2d6d4770f0018ce5445356fd180516077988822e222b24","bytes":9264,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_035_spectral.npz","sha256":"0353f44c6c3ac26f728ae663f9c729589662a7af51dbb66b374590827b1e4f40","bytes":4384,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_055_product.npz","sha256":"d25f8cfb654dd813ca7c1e1d78612127f54e4c8416024a71fe0706da167fef00","bytes":9387,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_055_spectral.npz","sha256":"44a7bd70a6ca12e179974b0f31df2ad991498c57ccc72ef713a7765c618bd2e2","bytes":4363,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_075_product.npz","sha256":"89256f8394b1d41ea5af31680a38c6a5062186bdfc91e6be9dce5a4a52699e9c","bytes":9470,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_075_spectral.npz","sha256":"afaff5cd316ea57d0d369f088932d2a0e94b623885cfdac569bb0dfb19a2fbad","bytes":4440,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_095_product.npz","sha256":"4a160a7248627cd10d1aa3fdf998098ece5928600740387373bb3c0b1bcd6ed8","bytes":9554,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_095_spectral.npz","sha256":"bdfb98de6b4f5cde4ccbf22cd432b70d0d4a1b48299035baa8aacc47f69ef5a6","bytes":4457,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_115_product.npz","sha256":"dfac5f73dfc7d92a603342ad4ab273480ea6616fcf44c809c42c7960e345819d","bytes":9547,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_115_spectral.npz","sha256":"9fc526419d0bc4a617b666d86d5946a8533d480f7eab96f12d890cbb74eb2fdd","bytes":4460,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_135_product.npz","sha256":"58afc01ca189a4abdd8e25fe10f7dd2a6f7816959f0a229884a7542975c669fa","bytes":9659,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_135_spectral.npz","sha256":"075593bc08db35adb694f12166e22153e251c46bfbd2781dc88f5af21f591237","bytes":4466,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_155_product.npz","sha256":"d55aa92ae94d9f1f804710749225da7f72a976d3b0ec249bfc02d7ad3dd2795c","bytes":9621,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_155_spectral.npz","sha256":"344381abe950e13422a64629d8da609ce06b93964429509d9066f912fab6c47c","bytes":4458,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_175_product.npz","sha256":"e0c5b579549d491ca63b3f53dfb7159fd3fe326b3fb1e06159a4de7f7cbcf645","bytes":9586,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_175_spectral.npz","sha256":"604d601ecf4ee2b4f8a3fd3e891a673486cfe7076dc82ce2c4d38fc2c597107a","bytes":4468,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_195_product.npz","sha256":"5112b72d41bfdab830f4ba7f847dea381354035291f188d3f1f6d03759f4aebf","bytes":9667,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/equilibrium_195_spectral.npz","sha256":"aecc55951110798c43b58fdb4c056bcfa5b9abb83027e900e4f436f8e0dae468","bytes":4458,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/rare_tail_10000_product.npz","sha256":"a9794ce82faf65f1a761348045ba1916b6d3ee54f19fb39a75634d657f84610b","bytes":7745,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/rare_tail_100000_product.npz","sha256":"95929b859c040df4b705410f53a547cf1864ddd446006a87e9069a6c332f28e6","bytes":8650,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/rare_tail_1000000_product.npz","sha256":"32e625dd99b5f7b19cfbf4fc7596a8501057a00bdd8ebae0880a4a5f0e85784a","bytes":9543,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/rare_tail_10000000_product.npz","sha256":"084ecbbb8de25dac6f20ec575b81fe1c54e2ae9fbd78ab14310feae016912ff5","bytes":10511,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/rare_tail_100000000_product.npz","sha256":"8fcd803caa1f54be96fd2f1c212a2c5ca35254bb286a76546934c3abb39b08fd","bytes":11228,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/thermal_000_spectral.npz","sha256":"92e785e7e8c03c7e8baacba5b3a64899e95402bb37a82bd3bf038ce1559853e1","bytes":42209,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/thermal_004_spectral.npz","sha256":"d0a7092afbfd904ce0e8eccfd5c04ee4b7c291ac583cd91dd790e9a00c2e100f","bytes":41650,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/thermal_009_spectral.npz","sha256":"03b04a4771d607fec76531fecd6093f95c891aecb7e186522e685707e2fc9189","bytes":40935,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/thermal_015_spectral.npz","sha256":"5dcf767b8b90714c1d5a11fcb8a74a4a0e34d8532b1116f779676f31c7142aef","bytes":40548,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/thermal_023_spectral.npz","sha256":"09260e595391a941fb6d1eef3a2384559d46b53abdffc8fb599e4ca17303add6","bytes":39890,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/thermal_031_spectral.npz","sha256":"8916790c505e1502246d0d0c13a5d6c00f648db8ea93f9fe1b4944e01be3fabd","bytes":39376,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/thermal_042_spectral.npz","sha256":"78604692d09ce451ffbc187693783a24576ef25958bd494a6cc30df20dd31c13","bytes":38634,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/thermal_056_spectral.npz","sha256":"715435cff7fa46ef018b584c6f1c9fdb91393a8665d404101d4dd773b9e47728","bytes":37651,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/thermal_075_spectral.npz","sha256":"12bfa6dd6d5477c771e4d10965003878c806d2385bb7a2c84f2a9fd1addc76d6","bytes":36662,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/thermal_107_spectral.npz","sha256":"d24494145b55a6a166249871ceecb94455e0a7ee06839fa3942b93a97d09ede7","bytes":35604,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/monte_carlo/thermal_201_spectral.npz","sha256":"f871dbba7d59cb7ddab5900b501fa4073b99fcf694d9742ff932a90f4d98cc04","bytes":33684,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/q_fisher_example.json","sha256":"0464fa43b81adfffd36469f68d59e0d065c91b040e6b38ad4f70ee469ef7a217","bytes":332,"media_type":"application/json","license":"CC-BY-4.0"},{"path":"paper/source/data/q_root_batching.csv","sha256":"b832f2a885f5e1a69350995efb6938186aefd939fb4fa59430ed0da3e2fdfefc","bytes":60032,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/q_scaled_remainder.csv","sha256":"9a7c8aa398b4b2552416077f72e8a2c564f677a2486f417e8f2898be6ee35086","bytes":225053,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/readout_monte_carlo_summary.json","sha256":"d61b9cd6b93a1966897c7ecc9e6f6b815dc910089127aa408b7e118a6bc6a49c","bytes":21724,"media_type":"application/json","license":"CC-BY-4.0"},{"path":"paper/source/data/readout_monte_carlo.csv","sha256":"312a98aac9e7e3ae8a4915436cbdcdb612024080c2790191e41e33aedbccf10d","bytes":417582,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/readout_noise_summary.json","sha256":"f8a117dd5d457264d06d1101657a1317b7d4d1aef757c3e2072766b0b20de0b2","bytes":773,"media_type":"application/json","license":"CC-BY-4.0"},{"path":"paper/source/data/receiver_design.json","sha256":"b2103752c8524dc9240ac4394ddae3fb0f5f53cd9679eda94e9e55f80f77ef88","bytes":3755,"media_type":"application/json","license":"CC-BY-4.0"},{"path":"paper/source/data/receiver_precision.csv","sha256":"2220ff20a27f4973a737e85f68c304e6afd3f53e82783214363fd59084026f6c","bytes":35159,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/receiver_validation.csv","sha256":"39e696e8f50875079f5854f34268119a02ce8674fce01f2bc97434dbf862671a","bytes":18149,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/score_tolerance.csv","sha256":"e7b1334fbaab74f8af56f957a3b11b9c179e86587ade307ef66986d464ebd263","bytes":10099,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/thermal_drive.csv","sha256":"8a723c4871a64ff822bff6ea673c09f8f1e4ee5e938b0bbeb9455a21131c4524","bytes":50172,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/thermo_dephasing_trajectory.csv","sha256":"d852c6921b459ad8418e691f4333d34b0b640bee7fcb75ff7c654662bb3a307a","bytes":75438,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/thermo_gap_dephasing.csv","sha256":"010778232690ecb03945ddc0c527f4ef5713de71a31cc7c659d8a9065a4abc78","bytes":18936,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/thermo_joint_score.npz","sha256":"fe9e9c467d829dde637bad1690efe56d7bb9791a252e920cc65146b2528537a9","bytes":903091,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/thermo_model_matrices.npz","sha256":"71e92db3185a033c71033a2fa9ae1ef23a95fde1cbd2c17ed4f775b3791e358d","bytes":10158,"media_type":"application/octet-stream","license":"CC0-1.0"},{"path":"paper/source/data/thermo_moment_bounds.csv","sha256":"8953a4f95eaa61906746540eea841f9e8e93ede08ee83b9247187e826ccc3b15","bytes":49893,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/thermo_noise_map.csv","sha256":"f8ac2f8c52397a5ce0c3cc5d685e782618c44b3478782424222c0b959e424e07","bytes":484628,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/thermo_parameter_map.csv","sha256":"40c5d23a496d4b5d0ae2df96a7e420ed1e24d4ded2e14dc96644c86e42325588","bytes":1453957,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/thermo_readout_noise.csv","sha256":"570c53af239735cc5f6522d2d9487d70d309cfef141286b17dad1053c194fa79","bytes":50332,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/thermo_size_check.csv","sha256":"d0d16ae7fea5448d44bfa5ac10f97c2d6b2171561fda1c4591201fce0a707b94","bytes":672,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/thermo_summary.json","sha256":"ed9862a5e1bced2b118d112e727280c9a80a2f85ba663bb50e2425fa8520cd4a","bytes":1238,"media_type":"application/json","license":"CC-BY-4.0"},{"path":"paper/source/data/thermo_work_distribution.csv","sha256":"424401f3f7acd117ee73b297d5d8cf32cf452d9e14c2ec2d72aa68fe335c43ae","bytes":32180,"media_type":"text/csv","license":"CC0-1.0"},{"path":"paper/source/data/worked_example.json","sha256":"46908fcc0938208a40f7e8bdcbfdd06a4ce874022caeb50cd30e49dca267f80f","bytes":434,"media_type":"application/json","license":"CC-BY-4.0"},{"path":"paper/source/figures/fig1_thermal_moments_dark.pdf","sha256":"a408047a0f124d4e69296d281f3c1399d53b9f1d83979740c5169d58025cc551","bytes":22235,"media_type":"application/pdf","license":"CC-BY-4.0"},{"path":"paper/source/figures/fig1_thermal_moments_dark.png","sha256":"fd42d67768c3c385cbdebe1f1f41650c425ab7b95514cc4caf910e6c4bed9895","bytes":100722,"media_type":"image/png","license":"CC-BY-4.0"},{"path":"paper/source/figures/fig1_thermal_moments.pdf","sha256":"269b89e1529d736d98b19a69da22cda330e7d015c52b820311e6f7a2e1cc10bd","bytes":22178,"media_type":"application/pdf","license":"CC-BY-4.0"},{"path":"paper/source/figures/fig1_thermal_moments.png","sha256":"ddfc272241611d7d374ea51873edded0d4f702093aec448df619914d72423c74","bytes":104367,"media_type":"image/png","license":"CC-BY-4.0"},{"path":"paper/source/figures/fig2_equilibrium_moments_dark.pdf","sha256":"ffff47f8239bebdeb497ac4e60396ccc9b626f5cab62594b6321936d335f6480","bytes":21843,"media_type":"application/pdf","license":"CC-BY-4.0"},{"path":"paper/source/figures/fig2_equilibrium_moments_dark.png","sha256":"938cedc1193a6ed6863608c6bcac5aae657bbfb879015a33e89299c5e157c212","bytes":120715,"media_type":"image/png","license":"CC-BY-4.0"},{"path":"paper/source/figures/fig2_equilibrium_moments.pdf","sha256":"2fe6f5244da2a306200510a8101495f5466c82a2874059b98455f1a5eed3e1b9","bytes":21792,"media_type":"application/pdf","license":"CC-BY-4.0"},{"path":"paper/source/figures/fig2_equilibrium_moments.png","sha256":"9eeee5fe55a9168b3fb755dab2aabb0d3cb6e8692a91ebef524940923e1ddbe5","bytes":126879,"media_type":"image/png","license":"CC-BY-4.0"},{"path":"paper/source/figures/supp_equilibrium_samples_dark.pdf","sha256":"49fa6305b27eb97716b72b47da33bfa049a6678c400cba25bd20bf64c612e63f","bytes":34471,"media_type":"application/pdf","license":"CC-BY-4.0"},{"path":"paper/source/figures/supp_equilibrium_samples_dark.png","sha256":"9f9603c330379628440461e2074b2c6d0d8929f632450e96c9d84ee83e4f603e","bytes":100492,"media_type":"image/png","license":"CC-BY-4.0"},{"path":"paper/source/figures/supp_equilibrium_samples.pdf","sha256":"f0bd290babda540c12b64e0d3ad4f93c658147bf9bb667be79b2a978816f32c0","bytes":34402,"media_type":"application/pdf","license":"CC-BY-4.0"},{"path":"paper/source/figures/supp_equilibrium_samples.png","sha256":"7af2ab80fc32bcba97017db4449a85d48a9ab7e70a6258e7ea07b430d82332a7","bytes":107705,"media_type":"image/png","license":"CC-BY-4.0"},{"path":"paper/source/figures/supp_thermal_samples_dark.pdf","sha256":"88d865948602a658545dc33c33480b7f981e71d4156e4cb2ea5d38e68baadbbb","bytes":30728,"media_type":"application/pdf","license":"CC-BY-4.0"},{"path":"paper/source/figures/supp_thermal_samples_dark.png","sha256":"de555c5831d101e2853ff48ae0e4f65db884a0866a8a9cf945c8edde012acdcb","bytes":118319,"media_type":"image/png","license":"CC-BY-4.0"},{"path":"paper/source/figures/supp_thermal_samples.pdf","sha256":"6cdf0eb5a5b32665343a17df124aefb30e2c422fde09a89ebf21011dccb1de53","bytes":30648,"media_type":"application/pdf","license":"CC-BY-4.0"},{"path":"paper/source/figures/supp_thermal_samples.png","sha256":"624bc7762c8a4114b67c0d51187a88dc8da672dbcb8913c135b763bad5e52866","bytes":123347,"media_type":"image/png","license":"CC-BY-4.0"},{"path":"provenance/provenance-v1.0.json","sha256":"0daed96e23d55405a2697f3c2feffad63da3536f4f15ff4f0fe440b924ff1471","bytes":4795,"media_type":"application/json","license":"CC-BY-4.0"},{"path":"reconstruction/Containerfile","sha256":"87a95074d6c117944dc30a31c17f2c35a5033ab504216c4e535c2817006604a6","bytes":447,"media_type":"application/octet-stream","license":"CC-BY-4.0"},{"path":"reconstruction/reproduce.py","sha256":"f1c7d87e59e68c964bdd82d6139d86766f181584f9102c1be8d3605837d26af6","bytes":5058,"media_type":"text/x-python","license":"Apache-2.0"},{"path":"reconstruction/requirements-lock.txt","sha256":"b7d59aabc9b78a1c3d04f72b6b2586002242877a41b5935e7ab81aa40b0c28c7","bytes":60,"media_type":"text/plain","license":"CC-BY-4.0"},{"path":"replication/replication-v1.0.yaml","sha256":"6a1dee744d885204f815ff8c1c9c232487ab5d452d36221ed3e0c1775904f509","bytes":7991,"media_type":"application/yaml","license":"CC-BY-4.0"},{"path":"reproduction/reproduction-v1.0.yaml","sha256":"30024c9c6395f005b409a7fd9588921a1037b6d3e93edb84a7c9964321d96d17","bytes":5278,"media_type":"application/yaml","license":"CC-BY-4.0"},{"path":"reviews/review-v1.0.yaml","sha256":"9ccd2c5fcc6dd47ea345887d9cec92d0df93b179e437676f5de80eb1c65482cd","bytes":7011,"media_type":"application/yaml","license":"CC-BY-4.0"},{"path":"schema.org.jsonld","sha256":"6ea16bf1bd65dc92d75920341ec38441db9bae0f54ddcab6c65197ceedec10b4","bytes":1999,"media_type":"application/ld+json","license":"CC-BY-4.0"}],"release_digest":"927025669f5569885608e68f91d0cdf3db5ecea777b388234c173f3de34dd014","bundle_hashes":{"paper":"6b9b3adf59e59d7ce64ee4417c1f9495cd6b26242634a821f5e058836ca6da45","literature":"18971291b34d86c43cd19d44a44ee85dd37682686a65c4037292181adaff3e00","reviews":"0e2fa64d58a294b7aacefde747d47deeec66ffc7e1ad08e16a1b535bb1099066","replication":"6d45ceed567a3e3a7c3aecd78b58efe79d0ebd72dd8eea7e4212d119256e951e","provenance":"799a579e4e6817ba9528aa670b2f14274bf2a6c0f29ac39d9414d67dd41fecdc"},"gates":{"solver":"PASS","novelty_audit":"PASS","adversarial_review":"PASS","independent_reproduction":"PASS","computation_reproduction":"PASS","editorial_gate":"PASS","build_provenance":"PASS"},"public_artifacts":["claims","code","data","editorial_decision","figures","literature_audit","paper","provenance","release_manifest","replication","reproduction","review"],"doi":"10.5281/zenodo.23047668"}}}