{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:4N2WYDFM6TX5LPLNDUG4U3W5OY","short_pith_number":"pith:4N2WYDFM","canonical_record":{"source":{"id":"1311.0702","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-04T13:57:20Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"81771d15c018207607d778f0541143110ad6db2dd814ef7f93e6364a4aab35dd","abstract_canon_sha256":"909c8c734f5ecc857bd379544e2c02c2d0ff79452a1673434ee046d07547a0fd"},"schema_version":"1.0"},"canonical_sha256":"e3756c0cacf4efd5bd6d1d0dca6edd762b0a05892d66f865b0d3d195e83bcbb0","source":{"kind":"arxiv","id":"1311.0702","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.0702","created_at":"2026-05-18T03:08:05Z"},{"alias_kind":"arxiv_version","alias_value":"1311.0702v1","created_at":"2026-05-18T03:08:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.0702","created_at":"2026-05-18T03:08:05Z"},{"alias_kind":"pith_short_12","alias_value":"4N2WYDFM6TX5","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"4N2WYDFM6TX5LPLN","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"4N2WYDFM","created_at":"2026-05-18T12:27:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:4N2WYDFM6TX5LPLNDUG4U3W5OY","target":"record","payload":{"canonical_record":{"source":{"id":"1311.0702","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-04T13:57:20Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"81771d15c018207607d778f0541143110ad6db2dd814ef7f93e6364a4aab35dd","abstract_canon_sha256":"909c8c734f5ecc857bd379544e2c02c2d0ff79452a1673434ee046d07547a0fd"},"schema_version":"1.0"},"canonical_sha256":"e3756c0cacf4efd5bd6d1d0dca6edd762b0a05892d66f865b0d3d195e83bcbb0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:08:05.089713Z","signature_b64":"pdTpszJE862VMrHi4ZZIh4L3u6Xh/3XCaJuTXuwHNhJZ7oMG5lJVeN3aJ1u0jFE99Hvhv6m9J56AOr//pw0ABw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e3756c0cacf4efd5bd6d1d0dca6edd762b0a05892d66f865b0d3d195e83bcbb0","last_reissued_at":"2026-05-18T03:08:05.089002Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:08:05.089002Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1311.0702","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:08:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Psp4DuJAvmogPLy0jEKuDn3vDkpS2EXetpXTKoJUwVS0VHqQ78xvS5GIxjhk7C5EPQvKMip+WzxToYTT7+6rDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T12:06:29.564253Z"},"content_sha256":"b7aa64a286a5039a7f65665618361ada25606c3eedee9f00be5b907143745609","schema_version":"1.0","event_id":"sha256:b7aa64a286a5039a7f65665618361ada25606c3eedee9f00be5b907143745609"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:4N2WYDFM6TX5LPLNDUG4U3W5OY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On two- and three-point functions of Landau gauge Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"Lorenz von Smekal, Markus Q. Huber","submitted_at":"2013-11-04T13:57:20Z","abstract_excerpt":"We present results for the gluon and ghost propagators and the ghost-gluon vertex obtained from Dyson-Schwinger equations. In the zero temperature case we elaborate on the role of the three-gluon vertex and discuss a model that can capture its qualitative features like its anomalous dimensions and a zero crossing of the dressing function. Our results compare well with lattice data. At non-zero temperature we calculated the ghost propagator which agrees rather well with lattice results already within our simple truncation. These results are used to obtain the temperature dependence of the ghost"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.0702","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:08:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4hoopl89z1XfQEwb6L+6NslEPy91JQV4aZeucI9MTpobLCdda4D1iOlVTbLv4yuIMXWsSM2pZE2HLkfJ2mHADQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T12:06:29.564839Z"},"content_sha256":"fb23f8efbcd735261f7fb4a585f875028d8e07be2189cf53540f28870038b214","schema_version":"1.0","event_id":"sha256:fb23f8efbcd735261f7fb4a585f875028d8e07be2189cf53540f28870038b214"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4N2WYDFM6TX5LPLNDUG4U3W5OY/bundle.json","state_url":"https://pith.science/pith/4N2WYDFM6TX5LPLNDUG4U3W5OY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4N2WYDFM6TX5LPLNDUG4U3W5OY/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":"2026-06-02T12:06:29Z","links":{"resolver":"https://pith.science/pith/4N2WYDFM6TX5LPLNDUG4U3W5OY","bundle":"https://pith.science/pith/4N2WYDFM6TX5LPLNDUG4U3W5OY/bundle.json","state":"https://pith.science/pith/4N2WYDFM6TX5LPLNDUG4U3W5OY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4N2WYDFM6TX5LPLNDUG4U3W5OY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:4N2WYDFM6TX5LPLNDUG4U3W5OY","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":"909c8c734f5ecc857bd379544e2c02c2d0ff79452a1673434ee046d07547a0fd","cross_cats_sorted":["hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-04T13:57:20Z","title_canon_sha256":"81771d15c018207607d778f0541143110ad6db2dd814ef7f93e6364a4aab35dd"},"schema_version":"1.0","source":{"id":"1311.0702","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.0702","created_at":"2026-05-18T03:08:05Z"},{"alias_kind":"arxiv_version","alias_value":"1311.0702v1","created_at":"2026-05-18T03:08:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.0702","created_at":"2026-05-18T03:08:05Z"},{"alias_kind":"pith_short_12","alias_value":"4N2WYDFM6TX5","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"4N2WYDFM6TX5LPLN","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"4N2WYDFM","created_at":"2026-05-18T12:27:34Z"}],"graph_snapshots":[{"event_id":"sha256:fb23f8efbcd735261f7fb4a585f875028d8e07be2189cf53540f28870038b214","target":"graph","created_at":"2026-05-18T03:08:05Z","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 present results for the gluon and ghost propagators and the ghost-gluon vertex obtained from Dyson-Schwinger equations. In the zero temperature case we elaborate on the role of the three-gluon vertex and discuss a model that can capture its qualitative features like its anomalous dimensions and a zero crossing of the dressing function. Our results compare well with lattice data. At non-zero temperature we calculated the ghost propagator which agrees rather well with lattice results already within our simple truncation. These results are used to obtain the temperature dependence of the ghost","authors_text":"Lorenz von Smekal, Markus Q. Huber","cross_cats":["hep-ph","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-04T13:57:20Z","title":"On two- and three-point functions of Landau gauge Yang-Mills theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.0702","kind":"arxiv","version":1},"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:b7aa64a286a5039a7f65665618361ada25606c3eedee9f00be5b907143745609","target":"record","created_at":"2026-05-18T03:08:05Z","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":"909c8c734f5ecc857bd379544e2c02c2d0ff79452a1673434ee046d07547a0fd","cross_cats_sorted":["hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-04T13:57:20Z","title_canon_sha256":"81771d15c018207607d778f0541143110ad6db2dd814ef7f93e6364a4aab35dd"},"schema_version":"1.0","source":{"id":"1311.0702","kind":"arxiv","version":1}},"canonical_sha256":"e3756c0cacf4efd5bd6d1d0dca6edd762b0a05892d66f865b0d3d195e83bcbb0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e3756c0cacf4efd5bd6d1d0dca6edd762b0a05892d66f865b0d3d195e83bcbb0","first_computed_at":"2026-05-18T03:08:05.089002Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:08:05.089002Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pdTpszJE862VMrHi4ZZIh4L3u6Xh/3XCaJuTXuwHNhJZ7oMG5lJVeN3aJ1u0jFE99Hvhv6m9J56AOr//pw0ABw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:08:05.089713Z","signed_message":"canonical_sha256_bytes"},"source_id":"1311.0702","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b7aa64a286a5039a7f65665618361ada25606c3eedee9f00be5b907143745609","sha256:fb23f8efbcd735261f7fb4a585f875028d8e07be2189cf53540f28870038b214"],"state_sha256":"9d977a9781ec5b9d6fd19ebdce494a004df18b52b029fea9f529c0c0fc0b555a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6XaB26ycroIfyG7ePDuDjTYI1u3b0MIa+7Y0cINHjdg90R0VOhhovtyu583UQaj7hw4/ijsnvyYO68pbs2pjAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T12:06:29.567701Z","bundle_sha256":"7f9c7d9766a019e1cf38110e350b331de16f52d381340122783fffeae06807d0"}}