{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:MWIDK3RXOU3KF36FXTKVDRJS7J","short_pith_number":"pith:MWIDK3RX","canonical_record":{"source":{"id":"1807.02907","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-07-09T01:28:20Z","cross_cats_sorted":[],"title_canon_sha256":"b83ece51be61875f4ec74069468324f04342b7a47719ef0d6a3ee14b1f41b043","abstract_canon_sha256":"3381bf72d3fba8c6f6b14a65135d3e4b6a452926fc5a2f017669bf163dbaef87"},"schema_version":"1.0"},"canonical_sha256":"6590356e377536a2efc5bcd551c532fa5e030c4fc42588796ac00abb27820d5a","source":{"kind":"arxiv","id":"1807.02907","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.02907","created_at":"2026-05-18T00:00:52Z"},{"alias_kind":"arxiv_version","alias_value":"1807.02907v2","created_at":"2026-05-18T00:00:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.02907","created_at":"2026-05-18T00:00:52Z"},{"alias_kind":"pith_short_12","alias_value":"MWIDK3RXOU3K","created_at":"2026-05-18T12:32:40Z"},{"alias_kind":"pith_short_16","alias_value":"MWIDK3RXOU3KF36F","created_at":"2026-05-18T12:32:40Z"},{"alias_kind":"pith_short_8","alias_value":"MWIDK3RX","created_at":"2026-05-18T12:32:40Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:MWIDK3RXOU3KF36FXTKVDRJS7J","target":"record","payload":{"canonical_record":{"source":{"id":"1807.02907","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-07-09T01:28:20Z","cross_cats_sorted":[],"title_canon_sha256":"b83ece51be61875f4ec74069468324f04342b7a47719ef0d6a3ee14b1f41b043","abstract_canon_sha256":"3381bf72d3fba8c6f6b14a65135d3e4b6a452926fc5a2f017669bf163dbaef87"},"schema_version":"1.0"},"canonical_sha256":"6590356e377536a2efc5bcd551c532fa5e030c4fc42588796ac00abb27820d5a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:00:52.371485Z","signature_b64":"i/HKjVXjcL1on9Ta3a+gb37w6Eu5RGBANJqgAD1z7ZBChJVKXemKvFZMB5dIDQUGA8U/WIlY3nEVSnVYiFLUAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6590356e377536a2efc5bcd551c532fa5e030c4fc42588796ac00abb27820d5a","last_reissued_at":"2026-05-18T00:00:52.370966Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:00:52.370966Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1807.02907","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:00:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+el/jZCyIjWg5QE/dnPHYOObp0b0+cTp0Vbw6N3N5XiXbfVdGLuTleyvk3xHB5bGK1gYw0Mga6QbL26d72UbDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T07:16:39.996068Z"},"content_sha256":"05064ab129d156683a1522530ea56df8c5b70875d8b45891ce486c316384028a","schema_version":"1.0","event_id":"sha256:05064ab129d156683a1522530ea56df8c5b70875d8b45891ce486c316384028a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:MWIDK3RXOU3KF36FXTKVDRJS7J","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Remarks on the static potential in theories with Lorentz violation terms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jos\\'e A. Helay\\\"el-Neto, Patricio Gaete","submitted_at":"2018-07-09T01:28:20Z","abstract_excerpt":"We study the impact of Lorentz violating terms on a physical observable for both electrodynamics of chiral matter and an Abelian Higgs-like model in $3+1$ dimensions. Our calculation is done within the framework of the gauge-invariant, but path-dependent, variables formalism. Interestingly enough, for electrodynamics of chiral matter we obtain a logarithmic correction to the usual static Coulomb potential. Whereas for a Abelian Higgs model with a Lorentz-breaking term, our result displays new corrections to the Yukawa potential."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.02907","kind":"arxiv","version":2},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:00:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UO/UdoOH++zi7+1WqedqDRnpXboB4yV02GAPHCtBAsoviRW+P1cJVzujreFjfcfHqNl/wL21g18YyJP5AzS6Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T07:16:39.996417Z"},"content_sha256":"280f29e23aadeec162bc95be2a724c537fe3d940a48f3a1c8ff02cc4f74f135e","schema_version":"1.0","event_id":"sha256:280f29e23aadeec162bc95be2a724c537fe3d940a48f3a1c8ff02cc4f74f135e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MWIDK3RXOU3KF36FXTKVDRJS7J/bundle.json","state_url":"https://pith.science/pith/MWIDK3RXOU3KF36FXTKVDRJS7J/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MWIDK3RXOU3KF36FXTKVDRJS7J/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":"2026-06-27T07:16:39Z","links":{"resolver":"https://pith.science/pith/MWIDK3RXOU3KF36FXTKVDRJS7J","bundle":"https://pith.science/pith/MWIDK3RXOU3KF36FXTKVDRJS7J/bundle.json","state":"https://pith.science/pith/MWIDK3RXOU3KF36FXTKVDRJS7J/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MWIDK3RXOU3KF36FXTKVDRJS7J/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:MWIDK3RXOU3KF36FXTKVDRJS7J","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":"3381bf72d3fba8c6f6b14a65135d3e4b6a452926fc5a2f017669bf163dbaef87","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-07-09T01:28:20Z","title_canon_sha256":"b83ece51be61875f4ec74069468324f04342b7a47719ef0d6a3ee14b1f41b043"},"schema_version":"1.0","source":{"id":"1807.02907","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.02907","created_at":"2026-05-18T00:00:52Z"},{"alias_kind":"arxiv_version","alias_value":"1807.02907v2","created_at":"2026-05-18T00:00:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.02907","created_at":"2026-05-18T00:00:52Z"},{"alias_kind":"pith_short_12","alias_value":"MWIDK3RXOU3K","created_at":"2026-05-18T12:32:40Z"},{"alias_kind":"pith_short_16","alias_value":"MWIDK3RXOU3KF36F","created_at":"2026-05-18T12:32:40Z"},{"alias_kind":"pith_short_8","alias_value":"MWIDK3RX","created_at":"2026-05-18T12:32:40Z"}],"graph_snapshots":[{"event_id":"sha256:280f29e23aadeec162bc95be2a724c537fe3d940a48f3a1c8ff02cc4f74f135e","target":"graph","created_at":"2026-05-18T00:00:52Z","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":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We study the impact of Lorentz violating terms on a physical observable for both electrodynamics of chiral matter and an Abelian Higgs-like model in $3+1$ dimensions. Our calculation is done within the framework of the gauge-invariant, but path-dependent, variables formalism. Interestingly enough, for electrodynamics of chiral matter we obtain a logarithmic correction to the usual static Coulomb potential. Whereas for a Abelian Higgs model with a Lorentz-breaking term, our result displays new corrections to the Yukawa potential.","authors_text":"Jos\\'e A. Helay\\\"el-Neto, Patricio Gaete","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-07-09T01:28:20Z","title":"Remarks on the static potential in theories with Lorentz violation terms"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.02907","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:05064ab129d156683a1522530ea56df8c5b70875d8b45891ce486c316384028a","target":"record","created_at":"2026-05-18T00:00:52Z","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":"3381bf72d3fba8c6f6b14a65135d3e4b6a452926fc5a2f017669bf163dbaef87","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-07-09T01:28:20Z","title_canon_sha256":"b83ece51be61875f4ec74069468324f04342b7a47719ef0d6a3ee14b1f41b043"},"schema_version":"1.0","source":{"id":"1807.02907","kind":"arxiv","version":2}},"canonical_sha256":"6590356e377536a2efc5bcd551c532fa5e030c4fc42588796ac00abb27820d5a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6590356e377536a2efc5bcd551c532fa5e030c4fc42588796ac00abb27820d5a","first_computed_at":"2026-05-18T00:00:52.370966Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:00:52.370966Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"i/HKjVXjcL1on9Ta3a+gb37w6Eu5RGBANJqgAD1z7ZBChJVKXemKvFZMB5dIDQUGA8U/WIlY3nEVSnVYiFLUAg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:00:52.371485Z","signed_message":"canonical_sha256_bytes"},"source_id":"1807.02907","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:05064ab129d156683a1522530ea56df8c5b70875d8b45891ce486c316384028a","sha256:280f29e23aadeec162bc95be2a724c537fe3d940a48f3a1c8ff02cc4f74f135e"],"state_sha256":"d73c2a2f78020b419670189da59718049d489155850c1f5f1c60a4757fd04c52"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LpWabMGbcHHWf+q9xRNSPzgGTAbVB8W+LOEaRqP02idurwIDfvEjHbmGeegWSaSVZzuVlDYQMcm/UP2aEtZ+Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-27T07:16:39.998305Z","bundle_sha256":"219d62d983c9a0b8f1dfdbd10eae60a9c119343ccb11694120d13d10dc0c647f"}}