{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:J7VM4J7AT5HW2PFBF5ZJGKG4E6","short_pith_number":"pith:J7VM4J7A","canonical_record":{"source":{"id":"2501.16721","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2025-01-28T05:58:15Z","cross_cats_sorted":["math.ST","physics.app-ph","stat.TH"],"title_canon_sha256":"0f712c5470ba9e559ef0ca23595c571ce3f933ff8060cd640d9376ae1ccfd1bc","abstract_canon_sha256":"75741242d58e5912b114c9dfff1a65f3dcf805d71ebd64d666ad2c558c54555e"},"schema_version":"1.0"},"canonical_sha256":"4feace27e09f4f6d3ca12f729328dc27b025b92c1ac27bbef718a45b8f7e2ac5","source":{"kind":"arxiv","id":"2501.16721","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.16721","created_at":"2026-05-28T01:04:26Z"},{"alias_kind":"arxiv_version","alias_value":"2501.16721v3","created_at":"2026-05-28T01:04:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.16721","created_at":"2026-05-28T01:04:26Z"},{"alias_kind":"pith_short_12","alias_value":"J7VM4J7AT5HW","created_at":"2026-05-28T01:04:26Z"},{"alias_kind":"pith_short_16","alias_value":"J7VM4J7AT5HW2PFB","created_at":"2026-05-28T01:04:26Z"},{"alias_kind":"pith_short_8","alias_value":"J7VM4J7A","created_at":"2026-05-28T01:04:26Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:J7VM4J7AT5HW2PFBF5ZJGKG4E6","target":"record","payload":{"canonical_record":{"source":{"id":"2501.16721","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2025-01-28T05:58:15Z","cross_cats_sorted":["math.ST","physics.app-ph","stat.TH"],"title_canon_sha256":"0f712c5470ba9e559ef0ca23595c571ce3f933ff8060cd640d9376ae1ccfd1bc","abstract_canon_sha256":"75741242d58e5912b114c9dfff1a65f3dcf805d71ebd64d666ad2c558c54555e"},"schema_version":"1.0"},"canonical_sha256":"4feace27e09f4f6d3ca12f729328dc27b025b92c1ac27bbef718a45b8f7e2ac5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-28T01:04:26.551448Z","signature_b64":"eClz0HWqzjVQa2pdOsvn080AA8oYkdC99uKtS35sXlI/tMJrpxCjXK2mRJk7XrcSFfRs+oBTSFMMym4GOibAAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4feace27e09f4f6d3ca12f729328dc27b025b92c1ac27bbef718a45b8f7e2ac5","last_reissued_at":"2026-05-28T01:04:26.550930Z","signature_status":"signed_v1","first_computed_at":"2026-05-28T01:04:26.550930Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2501.16721","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-28T01:04:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iijoXTGjdc4It3gpk9p2uNZaebmp1XwouQEdg4KQ4l2Gm1pL+ECVZcrghXeKYlI4uc74nMGwW0tpP9xb+wrHCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T01:26:04.167192Z"},"content_sha256":"71453dda2c241b648efb2bb43e021895047edcf5df2e4bc1699b818fe069d7bc","schema_version":"1.0","event_id":"sha256:71453dda2c241b648efb2bb43e021895047edcf5df2e4bc1699b818fe069d7bc"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:J7VM4J7AT5HW2PFBF5ZJGKG4E6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Heat-dissipation decomposition and free-energy generation in a non-equilibrium dot with multi-electron states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"Decomposing total heat into housekeeping and excess parts in a driven nanodot shows direct correlation with generated free energy.","cross_cats":["math.ST","physics.app-ph","stat.TH"],"primary_cat":"cond-mat.stat-mech","authors_text":"Chloe Salhani, Katsuhiko Nishiguchi, Kensaku Chida, Takase Shimizu, Toshiaki Hayashi","submitted_at":"2025-01-28T05:58:15Z","abstract_excerpt":"We experimentally demonstrate the decomposition of heat dissipation during free-energy generation in a nanometer-scale dot transitioning to a non-equilibrium steady state via single-electron counting statistics. An alternating-current signal driving a reservoir that injects multiple electrons into the dot makes it non-equilibrium, leading to free-energy generation, heat dissipation, and Shannon-entropy production. By analyzing the time-domain probability distributions of multi-electron states of the dot, we quantitatively decompose the heat dissipation into housekeeping and excess heats, there"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"By analyzing the time-domain probability distributions of multi-electron states of the dot, we quantitatively decompose the heat dissipation into housekeeping and excess heats, thereby revealing their direct correlation with free-energy generation. This correlation suggests that the ratio of the generated free energy to the work applied to the dot can potentially reach 0.5 under far-from-equilibrium conditions induced by a large signal, while an efficiency of 0.25 was experimentally achieved.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"That the measured time-domain probability distributions of multi-electron states permit an accurate, quantitative separation of total heat into housekeeping and excess components without unaccounted systematic errors from the AC drive, finite measurement bandwidth, or multi-electron interactions.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Experimental decomposition of heat dissipation into housekeeping and excess components in a multi-electron quantum dot reveals correlation with free-energy generation, achieving 0.25 efficiency with potential for 0.5.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Decomposing total heat into housekeeping and excess parts in a driven nanodot shows direct correlation with generated free energy.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"c6593afe5080f64a9c8e20d33dc960c9333093b72526645a880cb3f7810b6014"},"source":{"id":"2501.16721","kind":"arxiv","version":3},"verdict":{"id":"07fe74df-49ec-438b-a723-76c80d3675c6","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-23T05:18:56.278073Z","strongest_claim":"By analyzing the time-domain probability distributions of multi-electron states of the dot, we quantitatively decompose the heat dissipation into housekeeping and excess heats, thereby revealing their direct correlation with free-energy generation. This correlation suggests that the ratio of the generated free energy to the work applied to the dot can potentially reach 0.5 under far-from-equilibrium conditions induced by a large signal, while an efficiency of 0.25 was experimentally achieved.","one_line_summary":"Experimental decomposition of heat dissipation into housekeeping and excess components in a multi-electron quantum dot reveals correlation with free-energy generation, achieving 0.25 efficiency with potential for 0.5.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"That the measured time-domain probability distributions of multi-electron states permit an accurate, quantitative separation of total heat into housekeeping and excess components without unaccounted systematic errors from the AC drive, finite measurement bandwidth, or multi-electron interactions.","pith_extraction_headline":"Decomposing total heat into housekeeping and excess parts in a driven nanodot shows direct correlation with generated free energy."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2501.16721/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":57,"sample":[{"doi":"","year":1961,"title":"Landauer, Irreversibility and heat generation in the computing process, IBM J","work_id":"1b4c2629-62a8-4d9f-9c74-cd16a34a4f6f","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2012,"title":"A. B´ erut, A. Arakelyan, A. Petrosyan, S. Ciliberto, R. Dillenschneider, and E. Lutz, Experimental verifica- tion of landauer’s principle linking information and ther- modynamics, Nature 483, 187 (201","work_id":"ed8e95d9-0234-4867-8434-e3fd43e44493","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2014,"title":"Y. Jun, M. c. v. Gavrilov, and J. Bechhoefer, High- precision test of landauer’s principle in a feedback trap, Phys. Rev. Lett. 113, 190601 (2014)","work_id":"75308ad7-385c-4270-b9bc-cdfe5be9c85e","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2014,"title":"J. V. Koski, V. F. Maisi, J. P. Pekola, and D. V. Averin, Experimental realization of a szilard engine with a single electron, Proc. Natl. Acad. Sci. USA 111, 13786 (2014)","work_id":"62b2efc9-ea0c-4b7d-8cdb-5f2d3fa56d95","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2015,"title":"A. B´ erut, A. Petrosyan, and S. Ciliberto, Information and thermodynamics: experimental verification of landauer’s erasure principle, J. Stat. Mech. 2015, P06015 (2015)","work_id":"e9f8b526-205a-425c-972d-f3da144aa4dc","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":57,"snapshot_sha256":"0dae1059e243226519c4b9aa7c8667e32b37d2c75ad4d38d6d1e2c9fe548635b","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"07fe74df-49ec-438b-a723-76c80d3675c6"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-28T01:04:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vswkzRC3AfMVK3kB7Vqgze9TZkYCWZDEteoIA64mslyoveLQsfMvCv/RgftyVdrD5QTR2ePA9N/z3TGpXQe3Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T01:26:04.168671Z"},"content_sha256":"54b08264f00a8befe67421a507be4b6a3780761b857d480a4a132a48328c999f","schema_version":"1.0","event_id":"sha256:54b08264f00a8befe67421a507be4b6a3780761b857d480a4a132a48328c999f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/J7VM4J7AT5HW2PFBF5ZJGKG4E6/bundle.json","state_url":"https://pith.science/pith/J7VM4J7AT5HW2PFBF5ZJGKG4E6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/J7VM4J7AT5HW2PFBF5ZJGKG4E6/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-12T01:26:04Z","links":{"resolver":"https://pith.science/pith/J7VM4J7AT5HW2PFBF5ZJGKG4E6","bundle":"https://pith.science/pith/J7VM4J7AT5HW2PFBF5ZJGKG4E6/bundle.json","state":"https://pith.science/pith/J7VM4J7AT5HW2PFBF5ZJGKG4E6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/J7VM4J7AT5HW2PFBF5ZJGKG4E6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:J7VM4J7AT5HW2PFBF5ZJGKG4E6","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"75741242d58e5912b114c9dfff1a65f3dcf805d71ebd64d666ad2c558c54555e","cross_cats_sorted":["math.ST","physics.app-ph","stat.TH"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2025-01-28T05:58:15Z","title_canon_sha256":"0f712c5470ba9e559ef0ca23595c571ce3f933ff8060cd640d9376ae1ccfd1bc"},"schema_version":"1.0","source":{"id":"2501.16721","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.16721","created_at":"2026-05-28T01:04:26Z"},{"alias_kind":"arxiv_version","alias_value":"2501.16721v3","created_at":"2026-05-28T01:04:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.16721","created_at":"2026-05-28T01:04:26Z"},{"alias_kind":"pith_short_12","alias_value":"J7VM4J7AT5HW","created_at":"2026-05-28T01:04:26Z"},{"alias_kind":"pith_short_16","alias_value":"J7VM4J7AT5HW2PFB","created_at":"2026-05-28T01:04:26Z"},{"alias_kind":"pith_short_8","alias_value":"J7VM4J7A","created_at":"2026-05-28T01:04:26Z"}],"graph_snapshots":[{"event_id":"sha256:54b08264f00a8befe67421a507be4b6a3780761b857d480a4a132a48328c999f","target":"graph","created_at":"2026-05-28T01:04:26Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"By analyzing the time-domain probability distributions of multi-electron states of the dot, we quantitatively decompose the heat dissipation into housekeeping and excess heats, thereby revealing their direct correlation with free-energy generation. This correlation suggests that the ratio of the generated free energy to the work applied to the dot can potentially reach 0.5 under far-from-equilibrium conditions induced by a large signal, while an efficiency of 0.25 was experimentally achieved."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"That the measured time-domain probability distributions of multi-electron states permit an accurate, quantitative separation of total heat into housekeeping and excess components without unaccounted systematic errors from the AC drive, finite measurement bandwidth, or multi-electron interactions."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Experimental decomposition of heat dissipation into housekeeping and excess components in a multi-electron quantum dot reveals correlation with free-energy generation, achieving 0.25 efficiency with potential for 0.5."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Decomposing total heat into housekeeping and excess parts in a driven nanodot shows direct correlation with generated free energy."}],"snapshot_sha256":"c6593afe5080f64a9c8e20d33dc960c9333093b72526645a880cb3f7810b6014"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2501.16721/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We experimentally demonstrate the decomposition of heat dissipation during free-energy generation in a nanometer-scale dot transitioning to a non-equilibrium steady state via single-electron counting statistics. An alternating-current signal driving a reservoir that injects multiple electrons into the dot makes it non-equilibrium, leading to free-energy generation, heat dissipation, and Shannon-entropy production. By analyzing the time-domain probability distributions of multi-electron states of the dot, we quantitatively decompose the heat dissipation into housekeeping and excess heats, there","authors_text":"Chloe Salhani, Katsuhiko Nishiguchi, Kensaku Chida, Takase Shimizu, Toshiaki Hayashi","cross_cats":["math.ST","physics.app-ph","stat.TH"],"headline":"Decomposing total heat into housekeeping and excess parts in a driven nanodot shows direct correlation with generated free energy.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2025-01-28T05:58:15Z","title":"Heat-dissipation decomposition and free-energy generation in a non-equilibrium dot with multi-electron states"},"references":{"count":57,"internal_anchors":0,"resolved_work":57,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"Landauer, Irreversibility and heat generation in the computing process, IBM J","work_id":"1b4c2629-62a8-4d9f-9c74-cd16a34a4f6f","year":1961},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"A. B´ erut, A. Arakelyan, A. Petrosyan, S. Ciliberto, R. Dillenschneider, and E. Lutz, Experimental verifica- tion of landauer’s principle linking information and ther- modynamics, Nature 483, 187 (201","work_id":"ed8e95d9-0234-4867-8434-e3fd43e44493","year":2012},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"Y. Jun, M. c. v. Gavrilov, and J. Bechhoefer, High- precision test of landauer’s principle in a feedback trap, Phys. Rev. Lett. 113, 190601 (2014)","work_id":"75308ad7-385c-4270-b9bc-cdfe5be9c85e","year":2014},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"J. V. Koski, V. F. Maisi, J. P. Pekola, and D. V. Averin, Experimental realization of a szilard engine with a single electron, Proc. Natl. Acad. Sci. USA 111, 13786 (2014)","work_id":"62b2efc9-ea0c-4b7d-8cdb-5f2d3fa56d95","year":2014},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"A. B´ erut, A. Petrosyan, and S. Ciliberto, Information and thermodynamics: experimental verification of landauer’s erasure principle, J. Stat. Mech. 2015, P06015 (2015)","work_id":"e9f8b526-205a-425c-972d-f3da144aa4dc","year":2015}],"snapshot_sha256":"0dae1059e243226519c4b9aa7c8667e32b37d2c75ad4d38d6d1e2c9fe548635b"},"source":{"id":"2501.16721","kind":"arxiv","version":3},"verdict":{"created_at":"2026-05-23T05:18:56.278073Z","id":"07fe74df-49ec-438b-a723-76c80d3675c6","model_set":{"reader":"grok-4.3"},"one_line_summary":"Experimental decomposition of heat dissipation into housekeeping and excess components in a multi-electron quantum dot reveals correlation with free-energy generation, achieving 0.25 efficiency with potential for 0.5.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Decomposing total heat into housekeeping and excess parts in a driven nanodot shows direct correlation with generated free energy.","strongest_claim":"By analyzing the time-domain probability distributions of multi-electron states of the dot, we quantitatively decompose the heat dissipation into housekeeping and excess heats, thereby revealing their direct correlation with free-energy generation. This correlation suggests that the ratio of the generated free energy to the work applied to the dot can potentially reach 0.5 under far-from-equilibrium conditions induced by a large signal, while an efficiency of 0.25 was experimentally achieved.","weakest_assumption":"That the measured time-domain probability distributions of multi-electron states permit an accurate, quantitative separation of total heat into housekeeping and excess components without unaccounted systematic errors from the AC drive, finite measurement bandwidth, or multi-electron interactions."}},"verdict_id":"07fe74df-49ec-438b-a723-76c80d3675c6"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:71453dda2c241b648efb2bb43e021895047edcf5df2e4bc1699b818fe069d7bc","target":"record","created_at":"2026-05-28T01:04:26Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"75741242d58e5912b114c9dfff1a65f3dcf805d71ebd64d666ad2c558c54555e","cross_cats_sorted":["math.ST","physics.app-ph","stat.TH"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2025-01-28T05:58:15Z","title_canon_sha256":"0f712c5470ba9e559ef0ca23595c571ce3f933ff8060cd640d9376ae1ccfd1bc"},"schema_version":"1.0","source":{"id":"2501.16721","kind":"arxiv","version":3}},"canonical_sha256":"4feace27e09f4f6d3ca12f729328dc27b025b92c1ac27bbef718a45b8f7e2ac5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4feace27e09f4f6d3ca12f729328dc27b025b92c1ac27bbef718a45b8f7e2ac5","first_computed_at":"2026-05-28T01:04:26.550930Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-28T01:04:26.550930Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"eClz0HWqzjVQa2pdOsvn080AA8oYkdC99uKtS35sXlI/tMJrpxCjXK2mRJk7XrcSFfRs+oBTSFMMym4GOibAAg==","signature_status":"signed_v1","signed_at":"2026-05-28T01:04:26.551448Z","signed_message":"canonical_sha256_bytes"},"source_id":"2501.16721","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:71453dda2c241b648efb2bb43e021895047edcf5df2e4bc1699b818fe069d7bc","sha256:54b08264f00a8befe67421a507be4b6a3780761b857d480a4a132a48328c999f"],"state_sha256":"283b908b1bb3f74dfe7aa99c037ec816129b671de739b73f495e2d914c964869"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WrH7XrK+xH5Sqym8KHfFCAhPZ7QO7akOo+p9yZDIIeYP4DzyYUndPqfrtVqwSKhtgmoUk8yJvPcbV80N8xubAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-12T01:26:04.173959Z","bundle_sha256":"aee8945d178ed71fa0be31fd4c19aeadcecbece66b50046380e6d50f0f870fad"}}