{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:OM2ULRAFWM6G7LU6O5EQYWMM7O","short_pith_number":"pith:OM2ULRAF","schema_version":"1.0","canonical_sha256":"733545c405b33c6fae9e77490c598cfbb18d249a0f6660935ab619dd8e3cccbe","source":{"kind":"arxiv","id":"0704.2308","version":1},"attestation_state":"computed","paper":{"title":"On dynamical gluon mass generation","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. C. Aguilar, J. Papavassiliou","submitted_at":"2007-04-18T10:02:15Z","abstract_excerpt":"The effective gluon propagator constructed with the pinch technique is governed by a Schwinger-Dyson equation with special structure and gauge properties, that can be deduced from the correspondence with the background field method. Most importantly the non-perturbative gluon self-energy is transverse order-by-order in the dressed loop expansion, and separately for gluonic and ghost contributions, a property which allows for a meanigfull truncation. A linearized version of the truncated Schwinger-Dyson equation is derived, using a vertex that satisfies the required Ward identity and contains m"},"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":"0704.2308","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2007-04-18T10:02:15Z","cross_cats_sorted":[],"title_canon_sha256":"f386050dbd38c813d2ce4830d1348c5a5514128f99faca3a8cc1adbc94d66097","abstract_canon_sha256":"5f167acdae30c473cd914a8918328ec874251df79e290fad78baa26965d85c60"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:16:19.516727Z","signature_b64":"DQXcRsbgnBxx7hPfhokOpzZHZKqIyd5ty1FRihlS4jpfubRNAUOPgeVydbcY2xvm6BN95/B6z7BjNcb7gsLrCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"733545c405b33c6fae9e77490c598cfbb18d249a0f6660935ab619dd8e3cccbe","last_reissued_at":"2026-07-04T15:16:19.516363Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:16:19.516363Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On dynamical gluon mass generation","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. C. Aguilar, J. Papavassiliou","submitted_at":"2007-04-18T10:02:15Z","abstract_excerpt":"The effective gluon propagator constructed with the pinch technique is governed by a Schwinger-Dyson equation with special structure and gauge properties, that can be deduced from the correspondence with the background field method. Most importantly the non-perturbative gluon self-energy is transverse order-by-order in the dressed loop expansion, and separately for gluonic and ghost contributions, a property which allows for a meanigfull truncation. A linearized version of the truncated Schwinger-Dyson equation is derived, using a vertex that satisfies the required Ward identity and contains m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0704.2308","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/0704.2308/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":"0704.2308","created_at":"2026-07-04T15:16:19.516427+00:00"},{"alias_kind":"arxiv_version","alias_value":"0704.2308v1","created_at":"2026-07-04T15:16:19.516427+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0704.2308","created_at":"2026-07-04T15:16:19.516427+00:00"},{"alias_kind":"pith_short_12","alias_value":"OM2ULRAFWM6G","created_at":"2026-07-04T15:16:19.516427+00:00"},{"alias_kind":"pith_short_16","alias_value":"OM2ULRAFWM6G7LU6","created_at":"2026-07-04T15:16:19.516427+00:00"},{"alias_kind":"pith_short_8","alias_value":"OM2ULRAF","created_at":"2026-07-04T15:16:19.516427+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/OM2ULRAFWM6G7LU6O5EQYWMM7O","json":"https://pith.science/pith/OM2ULRAFWM6G7LU6O5EQYWMM7O.json","graph_json":"https://pith.science/api/pith-number/OM2ULRAFWM6G7LU6O5EQYWMM7O/graph.json","events_json":"https://pith.science/api/pith-number/OM2ULRAFWM6G7LU6O5EQYWMM7O/events.json","paper":"https://pith.science/paper/OM2ULRAF"},"agent_actions":{"view_html":"https://pith.science/pith/OM2ULRAFWM6G7LU6O5EQYWMM7O","download_json":"https://pith.science/pith/OM2ULRAFWM6G7LU6O5EQYWMM7O.json","view_paper":"https://pith.science/paper/OM2ULRAF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0704.2308&json=true","fetch_graph":"https://pith.science/api/pith-number/OM2ULRAFWM6G7LU6O5EQYWMM7O/graph.json","fetch_events":"https://pith.science/api/pith-number/OM2ULRAFWM6G7LU6O5EQYWMM7O/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OM2ULRAFWM6G7LU6O5EQYWMM7O/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OM2ULRAFWM6G7LU6O5EQYWMM7O/action/storage_attestation","attest_author":"https://pith.science/pith/OM2ULRAFWM6G7LU6O5EQYWMM7O/action/author_attestation","sign_citation":"https://pith.science/pith/OM2ULRAFWM6G7LU6O5EQYWMM7O/action/citation_signature","submit_replication":"https://pith.science/pith/OM2ULRAFWM6G7LU6O5EQYWMM7O/action/replication_record"}},"created_at":"2026-07-04T15:16:19.516427+00:00","updated_at":"2026-07-04T15:16:19.516427+00:00"}