{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:4WQKZJ6JRTD6K6LH47XMPAFURM","short_pith_number":"pith:4WQKZJ6J","schema_version":"1.0","canonical_sha256":"e5a0aca7c98cc7e57967e7eec780b48b3dff0d00a727b2126e4bad56dff9e1c2","source":{"kind":"arxiv","id":"2301.00980","version":1},"attestation_state":"computed","paper":{"title":"The Thermal Substructure of General Relativity","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Manfred Requardt","submitted_at":"2023-01-03T07:19:50Z","abstract_excerpt":"In a first step we will provide arguments for the understanding of quantum space-time (QST), that means, the microscopic substructure which is assumed to underly ordinary smooth classical space-time, as a thermal system at each (macroscopic) point $x$ of the classical space-time manifold (ST). In this context we exploit among other things some recent findings in the foundations of quantum statistical mechanics.\n  We argue that the classical metric tensor field $g_{ij}(x)$ plays the role of an order parameter field, signalling the existence of a primordial phase transition in which both space-t"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2301.00980","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2023-01-03T07:19:50Z","cross_cats_sorted":[],"title_canon_sha256":"ace85cc3f0cf1be5aecf888f8e9fa6e5443417796f08d8b87e1fed9b02cdf0f0","abstract_canon_sha256":"16c1d6e9cfed94e6932dff8c0509591961b4208d7018a40e39d0f12b51685ac7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:29:58.153872Z","signature_b64":"8q9Ggp8udJKgp46QBWJqaojxqoSKeZ1Ji7JK6IAv0CbX2Qy6jf7h1ys5xRxneGRKkrXL43/rHpOThFQnVt2UAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e5a0aca7c98cc7e57967e7eec780b48b3dff0d00a727b2126e4bad56dff9e1c2","last_reissued_at":"2026-07-05T05:29:58.153387Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:29:58.153387Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Thermal Substructure of General Relativity","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Manfred Requardt","submitted_at":"2023-01-03T07:19:50Z","abstract_excerpt":"In a first step we will provide arguments for the understanding of quantum space-time (QST), that means, the microscopic substructure which is assumed to underly ordinary smooth classical space-time, as a thermal system at each (macroscopic) point $x$ of the classical space-time manifold (ST). In this context we exploit among other things some recent findings in the foundations of quantum statistical mechanics.\n  We argue that the classical metric tensor field $g_{ij}(x)$ plays the role of an order parameter field, signalling the existence of a primordial phase transition in which both space-t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2301.00980","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2301.00980/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2301.00980","created_at":"2026-07-05T05:29:58.153444+00:00"},{"alias_kind":"arxiv_version","alias_value":"2301.00980v1","created_at":"2026-07-05T05:29:58.153444+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2301.00980","created_at":"2026-07-05T05:29:58.153444+00:00"},{"alias_kind":"pith_short_12","alias_value":"4WQKZJ6JRTD6","created_at":"2026-07-05T05:29:58.153444+00:00"},{"alias_kind":"pith_short_16","alias_value":"4WQKZJ6JRTD6K6LH","created_at":"2026-07-05T05:29:58.153444+00:00"},{"alias_kind":"pith_short_8","alias_value":"4WQKZJ6J","created_at":"2026-07-05T05:29:58.153444+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.01419","citing_title":"The Crossed Product, Modular (Tomita) Dynamics and its Role in the Transition of Type $III$ to Type $II_{\\infty}$ v.Neumann Algebras and Connections to Quantum Gravity","ref_index":34,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4WQKZJ6JRTD6K6LH47XMPAFURM","json":"https://pith.science/pith/4WQKZJ6JRTD6K6LH47XMPAFURM.json","graph_json":"https://pith.science/api/pith-number/4WQKZJ6JRTD6K6LH47XMPAFURM/graph.json","events_json":"https://pith.science/api/pith-number/4WQKZJ6JRTD6K6LH47XMPAFURM/events.json","paper":"https://pith.science/paper/4WQKZJ6J"},"agent_actions":{"view_html":"https://pith.science/pith/4WQKZJ6JRTD6K6LH47XMPAFURM","download_json":"https://pith.science/pith/4WQKZJ6JRTD6K6LH47XMPAFURM.json","view_paper":"https://pith.science/paper/4WQKZJ6J","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2301.00980&json=true","fetch_graph":"https://pith.science/api/pith-number/4WQKZJ6JRTD6K6LH47XMPAFURM/graph.json","fetch_events":"https://pith.science/api/pith-number/4WQKZJ6JRTD6K6LH47XMPAFURM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4WQKZJ6JRTD6K6LH47XMPAFURM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4WQKZJ6JRTD6K6LH47XMPAFURM/action/storage_attestation","attest_author":"https://pith.science/pith/4WQKZJ6JRTD6K6LH47XMPAFURM/action/author_attestation","sign_citation":"https://pith.science/pith/4WQKZJ6JRTD6K6LH47XMPAFURM/action/citation_signature","submit_replication":"https://pith.science/pith/4WQKZJ6JRTD6K6LH47XMPAFURM/action/replication_record"}},"created_at":"2026-07-05T05:29:58.153444+00:00","updated_at":"2026-07-05T05:29:58.153444+00:00"}