{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:SD5N4XR3TQALRKL6CVGDLSNKKC","short_pith_number":"pith:SD5N4XR3","schema_version":"1.0","canonical_sha256":"90fade5e3b9c00b8a97e154c35c9aa50a5145f35855f895e6facb2854b38e05e","source":{"kind":"arxiv","id":"2608.04895","version":1},"attestation_state":"computed","paper":{"title":"Newtonian Potential in Weyl Gravitoelectromagnetism","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"A. F. Santos, L. A. S. Evangelista","submitted_at":"2026-08-05T14:21:46Z","abstract_excerpt":"The gauge structure of the Weyl Gravitoelectromagnetic (GEM) formalism has been investigated, showing that although the theory admits additional propagating modes, only an effective spin-2 sector contributes to physical observables. Building on this result, the formalism is applied to Bhabha scattering mediated by the tensor field $A_{\\mu\\nu}$, and the Newtonian gravitational potential is derived in the zero-temperature limit. Finite-temperature effects are incorporated through the Thermo Field Dynamics (TFD) formalism. While the Newtonian interaction is recovered at low temperatures, it becom"},"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":"2608.04895","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2026-08-05T14:21:46Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"3b40cf95acca837f5c3ae4abcafdf624e0c5320e58acbcf7bc66e7379e2d9cd7","abstract_canon_sha256":"0244ccc3c9ed6ff1cc31498c015552c4ae9ad07a1d1b6726abbdb6c698c12a0c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-06T01:47:35.585834Z","signature_b64":"N0V774E3HpSokTBmWGmCJk+fMUtzzutaztXO11NJUZsYHgLviz+2TqyoS3pqfOdt9hUXMLTe+eLChaxzl9dSCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"90fade5e3b9c00b8a97e154c35c9aa50a5145f35855f895e6facb2854b38e05e","last_reissued_at":"2026-08-06T01:47:35.584429Z","signature_status":"signed_v1","first_computed_at":"2026-08-06T01:47:35.584429Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Newtonian Potential in Weyl Gravitoelectromagnetism","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"A. F. Santos, L. A. S. Evangelista","submitted_at":"2026-08-05T14:21:46Z","abstract_excerpt":"The gauge structure of the Weyl Gravitoelectromagnetic (GEM) formalism has been investigated, showing that although the theory admits additional propagating modes, only an effective spin-2 sector contributes to physical observables. Building on this result, the formalism is applied to Bhabha scattering mediated by the tensor field $A_{\\mu\\nu}$, and the Newtonian gravitational potential is derived in the zero-temperature limit. Finite-temperature effects are incorporated through the Thermo Field Dynamics (TFD) formalism. While the Newtonian interaction is recovered at low temperatures, it becom"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.04895","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/2608.04895/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":"2608.04895","created_at":"2026-08-06T01:47:35.586243+00:00"},{"alias_kind":"arxiv_version","alias_value":"2608.04895v1","created_at":"2026-08-06T01:47:35.586243+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.04895","created_at":"2026-08-06T01:47:35.586243+00:00"},{"alias_kind":"pith_short_12","alias_value":"SD5N4XR3TQAL","created_at":"2026-08-06T01:47:35.586243+00:00"},{"alias_kind":"pith_short_16","alias_value":"SD5N4XR3TQALRKL6","created_at":"2026-08-06T01:47:35.586243+00:00"},{"alias_kind":"pith_short_8","alias_value":"SD5N4XR3","created_at":"2026-08-06T01:47:35.586243+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/SD5N4XR3TQALRKL6CVGDLSNKKC","json":"https://pith.science/pith/SD5N4XR3TQALRKL6CVGDLSNKKC.json","graph_json":"https://pith.science/api/pith-number/SD5N4XR3TQALRKL6CVGDLSNKKC/graph.json","events_json":"https://pith.science/api/pith-number/SD5N4XR3TQALRKL6CVGDLSNKKC/events.json","paper":"https://pith.science/paper/SD5N4XR3"},"agent_actions":{"view_html":"https://pith.science/pith/SD5N4XR3TQALRKL6CVGDLSNKKC","download_json":"https://pith.science/pith/SD5N4XR3TQALRKL6CVGDLSNKKC.json","view_paper":"https://pith.science/paper/SD5N4XR3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2608.04895&json=true","fetch_graph":"https://pith.science/api/pith-number/SD5N4XR3TQALRKL6CVGDLSNKKC/graph.json","fetch_events":"https://pith.science/api/pith-number/SD5N4XR3TQALRKL6CVGDLSNKKC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SD5N4XR3TQALRKL6CVGDLSNKKC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SD5N4XR3TQALRKL6CVGDLSNKKC/action/storage_attestation","attest_author":"https://pith.science/pith/SD5N4XR3TQALRKL6CVGDLSNKKC/action/author_attestation","sign_citation":"https://pith.science/pith/SD5N4XR3TQALRKL6CVGDLSNKKC/action/citation_signature","submit_replication":"https://pith.science/pith/SD5N4XR3TQALRKL6CVGDLSNKKC/action/replication_record"}},"created_at":"2026-08-06T01:47:35.586243+00:00","updated_at":"2026-08-06T01:47:35.586243+00:00"}