{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:GQNXHLKHJBHT5GXANGEM6KRF7U","short_pith_number":"pith:GQNXHLKH","canonical_record":{"source":{"id":"1401.0713","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-03T20:45:07Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"5c918bed363a744aaecd7a6d27b0e551b2d3951d35b914dee6aeca9fd7b2f971","abstract_canon_sha256":"f76c2cd7202c0a6f3bbbfa3e004d709ceac4d8439986ea982feea2a44e6c387a"},"schema_version":"1.0"},"canonical_sha256":"341b73ad47484f3e9ae06988cf2a25fd02f8ab347eeb3bff4484a1b9c49ed94a","source":{"kind":"arxiv","id":"1401.0713","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.0713","created_at":"2026-05-18T02:55:05Z"},{"alias_kind":"arxiv_version","alias_value":"1401.0713v2","created_at":"2026-05-18T02:55:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.0713","created_at":"2026-05-18T02:55:05Z"},{"alias_kind":"pith_short_12","alias_value":"GQNXHLKHJBHT","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_16","alias_value":"GQNXHLKHJBHT5GXA","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_8","alias_value":"GQNXHLKH","created_at":"2026-05-18T12:28:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:GQNXHLKHJBHT5GXANGEM6KRF7U","target":"record","payload":{"canonical_record":{"source":{"id":"1401.0713","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-03T20:45:07Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"5c918bed363a744aaecd7a6d27b0e551b2d3951d35b914dee6aeca9fd7b2f971","abstract_canon_sha256":"f76c2cd7202c0a6f3bbbfa3e004d709ceac4d8439986ea982feea2a44e6c387a"},"schema_version":"1.0"},"canonical_sha256":"341b73ad47484f3e9ae06988cf2a25fd02f8ab347eeb3bff4484a1b9c49ed94a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:55:05.598896Z","signature_b64":"bT+2bpYFrnE7YsDl9L1yask3bu7oV11MuKvP7MVy/e9RkiJgYqsB3WV0nPIBsDkjy2cmBC+t9wG19GJzujRUAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"341b73ad47484f3e9ae06988cf2a25fd02f8ab347eeb3bff4484a1b9c49ed94a","last_reissued_at":"2026-05-18T02:55:05.598384Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:55:05.598384Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1401.0713","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:55:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gJMzSFIIuugjUAbJVcy/IDHqjRj0ozl4r6DypI6q0p+Ht/RhnudzLae4dREfTcGdN5jbmlioYHGe+g6o5WPIDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T15:49:46.881416Z"},"content_sha256":"f42febf483e2607086192220d19288e6cc9f942ed773708b6b1e481e47082eee","schema_version":"1.0","event_id":"sha256:f42febf483e2607086192220d19288e6cc9f942ed773708b6b1e481e47082eee"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:GQNXHLKHJBHT5GXANGEM6KRF7U","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Gluonic three-point correlations in pure Landau gauge QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"Adrian L. Blum, Lorenz von Smekal, Mario Mitter, Markus Q. Huber","submitted_at":"2014-01-03T20:45:07Z","abstract_excerpt":"We report on the first self-consistent solution of the Dyson-Schwinger equation (DSE) for the three-gluon vertex. Based on earlier results for the propagators which match data from lattice Monte-Carlo simulations, we obtain results for the three-gluon vertex that are in very good agreement with available lattice data likewise. Feeding these results back into the propagator DSEs leads to some changes especially in the gluon propagator. These changes allow us to assess previously used models for the three-gluon vertex and to systematically estimate the influence of neglected two-loop diagrams wi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.0713","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:55:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mwuD3p8Z0PDnchZdSo4/kLOnVkrjdymIsVhLOqxsn2Gpob+3UepUi72hWOKlW+T6XaMLzPB8IUmlvEenE0PzCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T15:49:46.881773Z"},"content_sha256":"94fb115a8a5892cfb9a56ea4c833a8be53fa1267bf168ac66bea818d54199cb8","schema_version":"1.0","event_id":"sha256:94fb115a8a5892cfb9a56ea4c833a8be53fa1267bf168ac66bea818d54199cb8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GQNXHLKHJBHT5GXANGEM6KRF7U/bundle.json","state_url":"https://pith.science/pith/GQNXHLKHJBHT5GXANGEM6KRF7U/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GQNXHLKHJBHT5GXANGEM6KRF7U/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":"2026-06-02T15:49:46Z","links":{"resolver":"https://pith.science/pith/GQNXHLKHJBHT5GXANGEM6KRF7U","bundle":"https://pith.science/pith/GQNXHLKHJBHT5GXANGEM6KRF7U/bundle.json","state":"https://pith.science/pith/GQNXHLKHJBHT5GXANGEM6KRF7U/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GQNXHLKHJBHT5GXANGEM6KRF7U/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:GQNXHLKHJBHT5GXANGEM6KRF7U","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":"f76c2cd7202c0a6f3bbbfa3e004d709ceac4d8439986ea982feea2a44e6c387a","cross_cats_sorted":["hep-lat","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-03T20:45:07Z","title_canon_sha256":"5c918bed363a744aaecd7a6d27b0e551b2d3951d35b914dee6aeca9fd7b2f971"},"schema_version":"1.0","source":{"id":"1401.0713","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.0713","created_at":"2026-05-18T02:55:05Z"},{"alias_kind":"arxiv_version","alias_value":"1401.0713v2","created_at":"2026-05-18T02:55:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.0713","created_at":"2026-05-18T02:55:05Z"},{"alias_kind":"pith_short_12","alias_value":"GQNXHLKHJBHT","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_16","alias_value":"GQNXHLKHJBHT5GXA","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_8","alias_value":"GQNXHLKH","created_at":"2026-05-18T12:28:30Z"}],"graph_snapshots":[{"event_id":"sha256:94fb115a8a5892cfb9a56ea4c833a8be53fa1267bf168ac66bea818d54199cb8","target":"graph","created_at":"2026-05-18T02:55:05Z","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 report on the first self-consistent solution of the Dyson-Schwinger equation (DSE) for the three-gluon vertex. Based on earlier results for the propagators which match data from lattice Monte-Carlo simulations, we obtain results for the three-gluon vertex that are in very good agreement with available lattice data likewise. Feeding these results back into the propagator DSEs leads to some changes especially in the gluon propagator. These changes allow us to assess previously used models for the three-gluon vertex and to systematically estimate the influence of neglected two-loop diagrams wi","authors_text":"Adrian L. Blum, Lorenz von Smekal, Mario Mitter, Markus Q. Huber","cross_cats":["hep-lat","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-03T20:45:07Z","title":"Gluonic three-point correlations in pure Landau gauge QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.0713","kind":"arxiv","version":2},"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:f42febf483e2607086192220d19288e6cc9f942ed773708b6b1e481e47082eee","target":"record","created_at":"2026-05-18T02:55:05Z","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":"f76c2cd7202c0a6f3bbbfa3e004d709ceac4d8439986ea982feea2a44e6c387a","cross_cats_sorted":["hep-lat","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-03T20:45:07Z","title_canon_sha256":"5c918bed363a744aaecd7a6d27b0e551b2d3951d35b914dee6aeca9fd7b2f971"},"schema_version":"1.0","source":{"id":"1401.0713","kind":"arxiv","version":2}},"canonical_sha256":"341b73ad47484f3e9ae06988cf2a25fd02f8ab347eeb3bff4484a1b9c49ed94a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"341b73ad47484f3e9ae06988cf2a25fd02f8ab347eeb3bff4484a1b9c49ed94a","first_computed_at":"2026-05-18T02:55:05.598384Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:55:05.598384Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bT+2bpYFrnE7YsDl9L1yask3bu7oV11MuKvP7MVy/e9RkiJgYqsB3WV0nPIBsDkjy2cmBC+t9wG19GJzujRUAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:55:05.598896Z","signed_message":"canonical_sha256_bytes"},"source_id":"1401.0713","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f42febf483e2607086192220d19288e6cc9f942ed773708b6b1e481e47082eee","sha256:94fb115a8a5892cfb9a56ea4c833a8be53fa1267bf168ac66bea818d54199cb8"],"state_sha256":"0175c204cf0eeb6d8f6e5afb1acf429ed464acb5c823a0f354e3990e96f641be"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cTy/g8tfq1S22sRfememQ6RpeEKU0xAYsSYFgWq+GZ/1sq9HeI2HOULEtnvoUKhfhI7Zn0XnyvNrHtWPfs1WAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T15:49:46.883732Z","bundle_sha256":"15f08bb52937b79efc792b5f897b593505738a49c14f1064e5904af3c29b6ed1"}}