{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:YQTRSRKC7CJ62BTQFXJGF2KLO6","short_pith_number":"pith:YQTRSRKC","schema_version":"1.0","canonical_sha256":"c427194542f893ed06702dd262e94b77902e02a5bcbcc3b61ae66eb72a09e9f9","source":{"kind":"arxiv","id":"1110.6095","version":1},"attestation_state":"computed","paper":{"title":"A New Interpretation of Einstein's Cosmological Constant","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Thomas L. Wilson","submitted_at":"2011-10-25T21:24:20Z","abstract_excerpt":"A new approach to the cosmological constant problem is proposed by modifying Einstein's theory of general relativity, using instead a scalar-tensor theory of gravitation. This theory of gravity crucially incorporates the concept of quantum symmetry breaking. The role of the cosmological constant $\\lambda$ as a graviton mass in the weak-field limit is necessarily utilized. Because $\\lambda$ takes on two values as a broken symmetry, so does the graviton mass -- one of which cannot be zero. Gravity now exhibits both long- and short-range forces, by introducing hadron bags into strong interaction "},"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":"1110.6095","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-10-25T21:24:20Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"89ffd26ac5cce24cc83b917938e86333e4bc6595d24882a5f8f28da5e13d44b3","abstract_canon_sha256":"1319a105e7e580ccfb2ffa67780b1afebade03eeda8e9ece287920f42373a9d7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:10:09.669578Z","signature_b64":"RJtkP+PLYdrEVdlQE++FbqPzgDFzO0srsXOUiC7x2MNVcjrBCKNkf8FwN9qYn6p+OlyIVP94sZjHMXj2eJLSDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c427194542f893ed06702dd262e94b77902e02a5bcbcc3b61ae66eb72a09e9f9","last_reissued_at":"2026-05-18T04:10:09.668745Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:10:09.668745Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A New Interpretation of Einstein's Cosmological Constant","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Thomas L. Wilson","submitted_at":"2011-10-25T21:24:20Z","abstract_excerpt":"A new approach to the cosmological constant problem is proposed by modifying Einstein's theory of general relativity, using instead a scalar-tensor theory of gravitation. This theory of gravity crucially incorporates the concept of quantum symmetry breaking. The role of the cosmological constant $\\lambda$ as a graviton mass in the weak-field limit is necessarily utilized. Because $\\lambda$ takes on two values as a broken symmetry, so does the graviton mass -- one of which cannot be zero. Gravity now exhibits both long- and short-range forces, by introducing hadron bags into strong interaction "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.6095","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":""},"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":"1110.6095","created_at":"2026-05-18T04:10:09.668873+00:00"},{"alias_kind":"arxiv_version","alias_value":"1110.6095v1","created_at":"2026-05-18T04:10:09.668873+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.6095","created_at":"2026-05-18T04:10:09.668873+00:00"},{"alias_kind":"pith_short_12","alias_value":"YQTRSRKC7CJ6","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_16","alias_value":"YQTRSRKC7CJ62BTQ","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_8","alias_value":"YQTRSRKC","created_at":"2026-05-18T12:26:47.523578+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YQTRSRKC7CJ62BTQFXJGF2KLO6","json":"https://pith.science/pith/YQTRSRKC7CJ62BTQFXJGF2KLO6.json","graph_json":"https://pith.science/api/pith-number/YQTRSRKC7CJ62BTQFXJGF2KLO6/graph.json","events_json":"https://pith.science/api/pith-number/YQTRSRKC7CJ62BTQFXJGF2KLO6/events.json","paper":"https://pith.science/paper/YQTRSRKC"},"agent_actions":{"view_html":"https://pith.science/pith/YQTRSRKC7CJ62BTQFXJGF2KLO6","download_json":"https://pith.science/pith/YQTRSRKC7CJ62BTQFXJGF2KLO6.json","view_paper":"https://pith.science/paper/YQTRSRKC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1110.6095&json=true","fetch_graph":"https://pith.science/api/pith-number/YQTRSRKC7CJ62BTQFXJGF2KLO6/graph.json","fetch_events":"https://pith.science/api/pith-number/YQTRSRKC7CJ62BTQFXJGF2KLO6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YQTRSRKC7CJ62BTQFXJGF2KLO6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YQTRSRKC7CJ62BTQFXJGF2KLO6/action/storage_attestation","attest_author":"https://pith.science/pith/YQTRSRKC7CJ62BTQFXJGF2KLO6/action/author_attestation","sign_citation":"https://pith.science/pith/YQTRSRKC7CJ62BTQFXJGF2KLO6/action/citation_signature","submit_replication":"https://pith.science/pith/YQTRSRKC7CJ62BTQFXJGF2KLO6/action/replication_record"}},"created_at":"2026-05-18T04:10:09.668873+00:00","updated_at":"2026-05-18T04:10:09.668873+00:00"}