{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:GK2JEI7J7SKM4FKSP72ONJCNYS","short_pith_number":"pith:GK2JEI7J","schema_version":"1.0","canonical_sha256":"32b49223e9fc94ce15527ff4e6a44dc48b9d5b52d3769c110f87024eead1a1f3","source":{"kind":"arxiv","id":"1502.02998","version":2},"attestation_state":"computed","paper":{"title":"Non-minimal couplings in Randall-Sundrum Scenarios","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"C. R. Muniz, G. Alencar, R.N. Costa Filho, R. R. Landim","submitted_at":"2015-02-10T17:19:35Z","abstract_excerpt":"In this paper we propose a new way of obtaining four dimensional gauge invariant $U(n)$ gauge field from a bulk action. The results are valid for both Randall-Sundrum scenarios and are obtained without the introduction of other fields or new degrees of freedom. The model is based only in non-minimal couplings with the gravity field. We show that two non-minimal couplings are necessary, one with the field strength and the other with a mass term. Despite the loosing of five dimensional gauge invariance by the mass term a massless gauge field is obtained over the brane. To obtain this, we need of"},"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":"1502.02998","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-02-10T17:19:35Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"2d31425fa404d2ac2b82ea40c7fe5d3fc0b0e523eaf2bf1bd0eb6ad3bd3cc701","abstract_canon_sha256":"0fe531af0df72bbf477f08fdeb5e6fa3703359341742fb77562db4aca1a167d2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:31:45.649331Z","signature_b64":"KfV+ofYfwjHLGlkdEGUzsNZwci0Re0z9T71T/7WWWABN5gPp91WZM7uYUDlV2v4g2vmgI9oNgAOxHXiyx+VTCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"32b49223e9fc94ce15527ff4e6a44dc48b9d5b52d3769c110f87024eead1a1f3","last_reissued_at":"2026-05-18T01:31:45.648707Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:31:45.648707Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-minimal couplings in Randall-Sundrum Scenarios","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"C. R. Muniz, G. Alencar, R.N. Costa Filho, R. R. Landim","submitted_at":"2015-02-10T17:19:35Z","abstract_excerpt":"In this paper we propose a new way of obtaining four dimensional gauge invariant $U(n)$ gauge field from a bulk action. The results are valid for both Randall-Sundrum scenarios and are obtained without the introduction of other fields or new degrees of freedom. The model is based only in non-minimal couplings with the gravity field. We show that two non-minimal couplings are necessary, one with the field strength and the other with a mass term. Despite the loosing of five dimensional gauge invariance by the mass term a massless gauge field is obtained over the brane. To obtain this, we need of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.02998","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1502.02998","created_at":"2026-05-18T01:31:45.648796+00:00"},{"alias_kind":"arxiv_version","alias_value":"1502.02998v2","created_at":"2026-05-18T01:31:45.648796+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.02998","created_at":"2026-05-18T01:31:45.648796+00:00"},{"alias_kind":"pith_short_12","alias_value":"GK2JEI7J7SKM","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_16","alias_value":"GK2JEI7J7SKM4FKS","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_8","alias_value":"GK2JEI7J","created_at":"2026-05-18T12:29:22.688609+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/GK2JEI7J7SKM4FKSP72ONJCNYS","json":"https://pith.science/pith/GK2JEI7J7SKM4FKSP72ONJCNYS.json","graph_json":"https://pith.science/api/pith-number/GK2JEI7J7SKM4FKSP72ONJCNYS/graph.json","events_json":"https://pith.science/api/pith-number/GK2JEI7J7SKM4FKSP72ONJCNYS/events.json","paper":"https://pith.science/paper/GK2JEI7J"},"agent_actions":{"view_html":"https://pith.science/pith/GK2JEI7J7SKM4FKSP72ONJCNYS","download_json":"https://pith.science/pith/GK2JEI7J7SKM4FKSP72ONJCNYS.json","view_paper":"https://pith.science/paper/GK2JEI7J","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1502.02998&json=true","fetch_graph":"https://pith.science/api/pith-number/GK2JEI7J7SKM4FKSP72ONJCNYS/graph.json","fetch_events":"https://pith.science/api/pith-number/GK2JEI7J7SKM4FKSP72ONJCNYS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GK2JEI7J7SKM4FKSP72ONJCNYS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GK2JEI7J7SKM4FKSP72ONJCNYS/action/storage_attestation","attest_author":"https://pith.science/pith/GK2JEI7J7SKM4FKSP72ONJCNYS/action/author_attestation","sign_citation":"https://pith.science/pith/GK2JEI7J7SKM4FKSP72ONJCNYS/action/citation_signature","submit_replication":"https://pith.science/pith/GK2JEI7J7SKM4FKSP72ONJCNYS/action/replication_record"}},"created_at":"2026-05-18T01:31:45.648796+00:00","updated_at":"2026-05-18T01:31:45.648796+00:00"}