{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:N7PJTEF73ARZOOHC4ZG52U3VBL","short_pith_number":"pith:N7PJTEF7","schema_version":"1.0","canonical_sha256":"6fde9990bfd8239738e2e64ddd53750ad67045a7e9fe3ab4078463a8bb7c3914","source":{"kind":"arxiv","id":"hep-th/0403276","version":1},"attestation_state":"computed","paper":{"title":"Low-energy Moller scattering in a Maxwell-Chern-Simons Lorentz-violating planar model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Manoel M. Ferreira Jr (UFMA)","submitted_at":"2004-03-29T03:51:27Z","abstract_excerpt":"One starts from a planar Maxwell-Chern-Simons model endowed with a Lorentz-violating term. The Dirac sector is introduced exhibiting a Yukawa and a minimal coupling with the scalar scalar and the gauge fields, respectively. One then evaluates the electron-electron interaction as the Fourier transform of the Moller scattering amplitude carried out in the non-relativistic limit. In the case of a purely time-like background, the interaction potential can be exactly solved, exhibiting a typical massless behavior far from the origin. The scalar interaction potential is always attractive whereas the"},"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":"hep-th/0403276","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-03-29T03:51:27Z","cross_cats_sorted":[],"title_canon_sha256":"32284414509f736e8e93cdfb9fbb9e5ec090f223ee70aefe067bc43f8f81a648","abstract_canon_sha256":"2297667ba84639600621206e0203a8530b7e32a0ae37bba1615bad8cbc85149a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:48:45.221806Z","signature_b64":"P9MMvBIyuAOEIVd0n6cTv4/j55tzj0MKE8/Lssquu11J74p5OS7n3yxAFs37+ba/nxQT+0DbZIGvZAw/8zWQBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6fde9990bfd8239738e2e64ddd53750ad67045a7e9fe3ab4078463a8bb7c3914","last_reissued_at":"2026-07-04T16:48:45.221421Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:48:45.221421Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Low-energy Moller scattering in a Maxwell-Chern-Simons Lorentz-violating planar model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Manoel M. Ferreira Jr (UFMA)","submitted_at":"2004-03-29T03:51:27Z","abstract_excerpt":"One starts from a planar Maxwell-Chern-Simons model endowed with a Lorentz-violating term. The Dirac sector is introduced exhibiting a Yukawa and a minimal coupling with the scalar scalar and the gauge fields, respectively. One then evaluates the electron-electron interaction as the Fourier transform of the Moller scattering amplitude carried out in the non-relativistic limit. In the case of a purely time-like background, the interaction potential can be exactly solved, exhibiting a typical massless behavior far from the origin. The scalar interaction potential is always attractive whereas the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0403276","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/hep-th/0403276/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":"hep-th/0403276","created_at":"2026-07-04T16:48:45.221484+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0403276v1","created_at":"2026-07-04T16:48:45.221484+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0403276","created_at":"2026-07-04T16:48:45.221484+00:00"},{"alias_kind":"pith_short_12","alias_value":"N7PJTEF73ARZ","created_at":"2026-07-04T16:48:45.221484+00:00"},{"alias_kind":"pith_short_16","alias_value":"N7PJTEF73ARZOOHC","created_at":"2026-07-04T16:48:45.221484+00:00"},{"alias_kind":"pith_short_8","alias_value":"N7PJTEF7","created_at":"2026-07-04T16:48:45.221484+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/N7PJTEF73ARZOOHC4ZG52U3VBL","json":"https://pith.science/pith/N7PJTEF73ARZOOHC4ZG52U3VBL.json","graph_json":"https://pith.science/api/pith-number/N7PJTEF73ARZOOHC4ZG52U3VBL/graph.json","events_json":"https://pith.science/api/pith-number/N7PJTEF73ARZOOHC4ZG52U3VBL/events.json","paper":"https://pith.science/paper/N7PJTEF7"},"agent_actions":{"view_html":"https://pith.science/pith/N7PJTEF73ARZOOHC4ZG52U3VBL","download_json":"https://pith.science/pith/N7PJTEF73ARZOOHC4ZG52U3VBL.json","view_paper":"https://pith.science/paper/N7PJTEF7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0403276&json=true","fetch_graph":"https://pith.science/api/pith-number/N7PJTEF73ARZOOHC4ZG52U3VBL/graph.json","fetch_events":"https://pith.science/api/pith-number/N7PJTEF73ARZOOHC4ZG52U3VBL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/N7PJTEF73ARZOOHC4ZG52U3VBL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/N7PJTEF73ARZOOHC4ZG52U3VBL/action/storage_attestation","attest_author":"https://pith.science/pith/N7PJTEF73ARZOOHC4ZG52U3VBL/action/author_attestation","sign_citation":"https://pith.science/pith/N7PJTEF73ARZOOHC4ZG52U3VBL/action/citation_signature","submit_replication":"https://pith.science/pith/N7PJTEF73ARZOOHC4ZG52U3VBL/action/replication_record"}},"created_at":"2026-07-04T16:48:45.221484+00:00","updated_at":"2026-07-04T16:48:45.221484+00:00"}