{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:MLUWAEYE4VO7JVVFWVUYB33VT5","short_pith_number":"pith:MLUWAEYE","schema_version":"1.0","canonical_sha256":"62e9601304e55df4d6a5b56980ef759f414f0b4edec70875b32ba0e543bac61f","source":{"kind":"arxiv","id":"1010.2945","version":1},"attestation_state":"computed","paper":{"title":"The IR sector of QCD: lattice versus Schwinger-Dyson equations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Daniele Binosi","submitted_at":"2010-10-14T15:02:34Z","abstract_excerpt":"Important information about the infrared dynamics of QCD is encoded in the behavior of its (of-shell) Green's functions, most notably the gluon and the ghost propagators. Due to recent improvements in the quality of lattice data and the truncation schemes employed for the Schwinger-Dyson equations we have now reached a point where the interplay between these two non-perturbative tools can be most fruitful. In this talk several of the above points will be reviewed, with particular emphasis on the implications for the ghost sector, the non-perturbative effective charge of QCD, and the Kugo-Ojima"},"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":"1010.2945","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-10-14T15:02:34Z","cross_cats_sorted":[],"title_canon_sha256":"23cfd131287b7acce1e7db8e1060a7219f77a3406d1acad70e02a392913913cc","abstract_canon_sha256":"f621bd9a6fcedb4fcef621085f63c2d8812afee6a18152f193642d2d7d49dfd0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:30:25.568735Z","signature_b64":"Yic5EbQGHouHGck2/4HPSsvgZJacLgzbr0VehUVk8oKKVnmgs+MnU/VMn1cz69UzEJNvMXE4ojZYlb3rxEkzBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"62e9601304e55df4d6a5b56980ef759f414f0b4edec70875b32ba0e543bac61f","last_reissued_at":"2026-05-18T04:30:25.568266Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:30:25.568266Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The IR sector of QCD: lattice versus Schwinger-Dyson equations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Daniele Binosi","submitted_at":"2010-10-14T15:02:34Z","abstract_excerpt":"Important information about the infrared dynamics of QCD is encoded in the behavior of its (of-shell) Green's functions, most notably the gluon and the ghost propagators. Due to recent improvements in the quality of lattice data and the truncation schemes employed for the Schwinger-Dyson equations we have now reached a point where the interplay between these two non-perturbative tools can be most fruitful. In this talk several of the above points will be reviewed, with particular emphasis on the implications for the ghost sector, the non-perturbative effective charge of QCD, and the Kugo-Ojima"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.2945","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":"1010.2945","created_at":"2026-05-18T04:30:25.568351+00:00"},{"alias_kind":"arxiv_version","alias_value":"1010.2945v1","created_at":"2026-05-18T04:30:25.568351+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.2945","created_at":"2026-05-18T04:30:25.568351+00:00"},{"alias_kind":"pith_short_12","alias_value":"MLUWAEYE4VO7","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_16","alias_value":"MLUWAEYE4VO7JVVF","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_8","alias_value":"MLUWAEYE","created_at":"2026-05-18T12:26:10.704358+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/MLUWAEYE4VO7JVVFWVUYB33VT5","json":"https://pith.science/pith/MLUWAEYE4VO7JVVFWVUYB33VT5.json","graph_json":"https://pith.science/api/pith-number/MLUWAEYE4VO7JVVFWVUYB33VT5/graph.json","events_json":"https://pith.science/api/pith-number/MLUWAEYE4VO7JVVFWVUYB33VT5/events.json","paper":"https://pith.science/paper/MLUWAEYE"},"agent_actions":{"view_html":"https://pith.science/pith/MLUWAEYE4VO7JVVFWVUYB33VT5","download_json":"https://pith.science/pith/MLUWAEYE4VO7JVVFWVUYB33VT5.json","view_paper":"https://pith.science/paper/MLUWAEYE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1010.2945&json=true","fetch_graph":"https://pith.science/api/pith-number/MLUWAEYE4VO7JVVFWVUYB33VT5/graph.json","fetch_events":"https://pith.science/api/pith-number/MLUWAEYE4VO7JVVFWVUYB33VT5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MLUWAEYE4VO7JVVFWVUYB33VT5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MLUWAEYE4VO7JVVFWVUYB33VT5/action/storage_attestation","attest_author":"https://pith.science/pith/MLUWAEYE4VO7JVVFWVUYB33VT5/action/author_attestation","sign_citation":"https://pith.science/pith/MLUWAEYE4VO7JVVFWVUYB33VT5/action/citation_signature","submit_replication":"https://pith.science/pith/MLUWAEYE4VO7JVVFWVUYB33VT5/action/replication_record"}},"created_at":"2026-05-18T04:30:25.568351+00:00","updated_at":"2026-05-18T04:30:25.568351+00:00"}