{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:65O4YTJODMJCXLWI2MUSCPH5Q3","short_pith_number":"pith:65O4YTJO","schema_version":"1.0","canonical_sha256":"f75dcc4d2e1b122baec8d329213cfd86c5c78b16965193122f97d0e61f31d263","source":{"kind":"arxiv","id":"1506.00035","version":1},"attestation_state":"computed","paper":{"title":"The Yang-Mills gauge theory in DFR noncommutative space-time","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Everton M. C. Abreu, M. J. Neves","submitted_at":"2015-05-29T21:35:01Z","abstract_excerpt":"The Doplicher-Fredenhagen-Roberts (DFR) framework for noncommutative (NC) space-times is considered as an alternative approach to describe the physics of quantum gravity, for instance. In this formalism, the NC parameter, {\\it i.e.} $\\theta^{\\mu\\nu}$, is promoted to a coordinate of a new extended space-time. Consequently, we have a field theory in a space-time with spatial extra-dimensions. This new coordinate has a canonical momentum associated, where the effects of a new physics can emerge in the fields propagation along the extra-dimension. In this paper we introduce the gauge invariance in"},"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":"1506.00035","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-05-29T21:35:01Z","cross_cats_sorted":[],"title_canon_sha256":"c8c90a3fe90ad342285d13afd19ac980536f4ab2729dc3b708e65edad9daeb37","abstract_canon_sha256":"c80455c26bc60b93ba0ad2861305a38c79bad56ee39445495f1ae15936ddf410"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:55.636829Z","signature_b64":"TcRjETpNJ2e1KHkuyoAUAgFxTBql+ZePBAhml8twLp4jboUJmWJwRfuQF7IgmCFbMV8BNg+VR2blKyCpbjB9AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f75dcc4d2e1b122baec8d329213cfd86c5c78b16965193122f97d0e61f31d263","last_reissued_at":"2026-05-18T01:59:55.636242Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:55.636242Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Yang-Mills gauge theory in DFR noncommutative space-time","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Everton M. C. Abreu, M. J. Neves","submitted_at":"2015-05-29T21:35:01Z","abstract_excerpt":"The Doplicher-Fredenhagen-Roberts (DFR) framework for noncommutative (NC) space-times is considered as an alternative approach to describe the physics of quantum gravity, for instance. In this formalism, the NC parameter, {\\it i.e.} $\\theta^{\\mu\\nu}$, is promoted to a coordinate of a new extended space-time. Consequently, we have a field theory in a space-time with spatial extra-dimensions. This new coordinate has a canonical momentum associated, where the effects of a new physics can emerge in the fields propagation along the extra-dimension. In this paper we introduce the gauge invariance in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.00035","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":"1506.00035","created_at":"2026-05-18T01:59:55.636340+00:00"},{"alias_kind":"arxiv_version","alias_value":"1506.00035v1","created_at":"2026-05-18T01:59:55.636340+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.00035","created_at":"2026-05-18T01:59:55.636340+00:00"},{"alias_kind":"pith_short_12","alias_value":"65O4YTJODMJC","created_at":"2026-05-18T12:29:07.941421+00:00"},{"alias_kind":"pith_short_16","alias_value":"65O4YTJODMJCXLWI","created_at":"2026-05-18T12:29:07.941421+00:00"},{"alias_kind":"pith_short_8","alias_value":"65O4YTJO","created_at":"2026-05-18T12:29:07.941421+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/65O4YTJODMJCXLWI2MUSCPH5Q3","json":"https://pith.science/pith/65O4YTJODMJCXLWI2MUSCPH5Q3.json","graph_json":"https://pith.science/api/pith-number/65O4YTJODMJCXLWI2MUSCPH5Q3/graph.json","events_json":"https://pith.science/api/pith-number/65O4YTJODMJCXLWI2MUSCPH5Q3/events.json","paper":"https://pith.science/paper/65O4YTJO"},"agent_actions":{"view_html":"https://pith.science/pith/65O4YTJODMJCXLWI2MUSCPH5Q3","download_json":"https://pith.science/pith/65O4YTJODMJCXLWI2MUSCPH5Q3.json","view_paper":"https://pith.science/paper/65O4YTJO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1506.00035&json=true","fetch_graph":"https://pith.science/api/pith-number/65O4YTJODMJCXLWI2MUSCPH5Q3/graph.json","fetch_events":"https://pith.science/api/pith-number/65O4YTJODMJCXLWI2MUSCPH5Q3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/65O4YTJODMJCXLWI2MUSCPH5Q3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/65O4YTJODMJCXLWI2MUSCPH5Q3/action/storage_attestation","attest_author":"https://pith.science/pith/65O4YTJODMJCXLWI2MUSCPH5Q3/action/author_attestation","sign_citation":"https://pith.science/pith/65O4YTJODMJCXLWI2MUSCPH5Q3/action/citation_signature","submit_replication":"https://pith.science/pith/65O4YTJODMJCXLWI2MUSCPH5Q3/action/replication_record"}},"created_at":"2026-05-18T01:59:55.636340+00:00","updated_at":"2026-05-18T01:59:55.636340+00:00"}