{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:CJ2PJC7PNMLA4M5SHYW7DURC2U","short_pith_number":"pith:CJ2PJC7P","canonical_record":{"source":{"id":"1211.6092","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-11-26T20:55:49Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"90dc9cd5bf2c3d4585ceb0361e042eedb5dca0fe3e96abf5099b98e7df4c767f","abstract_canon_sha256":"d9a4d102181472e460a19ec607b0331423bd1eea62e13d8549c39033faaa291b"},"schema_version":"1.0"},"canonical_sha256":"1274f48bef6b160e33b23e2df1d222d51769240fc6d787789d886fbe1d9cd390","source":{"kind":"arxiv","id":"1211.6092","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.6092","created_at":"2026-05-18T03:20:09Z"},{"alias_kind":"arxiv_version","alias_value":"1211.6092v2","created_at":"2026-05-18T03:20:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.6092","created_at":"2026-05-18T03:20:09Z"},{"alias_kind":"pith_short_12","alias_value":"CJ2PJC7PNMLA","created_at":"2026-05-18T12:27:01Z"},{"alias_kind":"pith_short_16","alias_value":"CJ2PJC7PNMLA4M5S","created_at":"2026-05-18T12:27:01Z"},{"alias_kind":"pith_short_8","alias_value":"CJ2PJC7P","created_at":"2026-05-18T12:27:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:CJ2PJC7PNMLA4M5SHYW7DURC2U","target":"record","payload":{"canonical_record":{"source":{"id":"1211.6092","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-11-26T20:55:49Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"90dc9cd5bf2c3d4585ceb0361e042eedb5dca0fe3e96abf5099b98e7df4c767f","abstract_canon_sha256":"d9a4d102181472e460a19ec607b0331423bd1eea62e13d8549c39033faaa291b"},"schema_version":"1.0"},"canonical_sha256":"1274f48bef6b160e33b23e2df1d222d51769240fc6d787789d886fbe1d9cd390","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:20:09.472887Z","signature_b64":"mEQL/b+ZGIxU1SF0czDOxD+bx2DcqAVj2O+afKs1I8PRAr9X8+zztMRRaMB6T0JwtGvRmGIzT2VvAzPES846DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1274f48bef6b160e33b23e2df1d222d51769240fc6d787789d886fbe1d9cd390","last_reissued_at":"2026-05-18T03:20:09.472286Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:20:09.472286Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1211.6092","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":"2026-05-18T03:20:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pzzvCEmF30iXHZuHs5U4WoKVlkIN2FpA4p93En3ghjx8pNj61XlrwvWwekvl6oybfjhBP8pHEnuJPLmGNSMNAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T18:34:53.222045Z"},"content_sha256":"af9987b8327007a38371b043e806cc9b76280264470b8462856368554c0a63bd","schema_version":"1.0","event_id":"sha256:af9987b8327007a38371b043e806cc9b76280264470b8462856368554c0a63bd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:CJ2PJC7PNMLA4M5SHYW7DURC2U","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the influence of three-point functions on the propagators of Landau gauge Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"Lorenz von Smekal, Markus Q. Huber","submitted_at":"2012-11-26T20:55:49Z","abstract_excerpt":"We solve the Dyson-Schwinger equations of the ghost and gluon propagators of Landau gauge Yang-Mills theory together with that of the ghost-gluon vertex. The latter plays a central role in many truncation schemes for functional equations. By including it dynamically we can determine its influence on the propagators. We also suggest a new model for the three-gluon vertex motivated by lattice data which plays a crucial role to obtain stable solutions when the ghost-gluon vertex is included. We find that both vertices have a sizable quantitative impact on the mid-momentum regime and contribute to"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.6092","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":"2026-05-18T03:20:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MjkXOMUHE2ihhbJwZHdTt2+8HP/AqqnPeEw132tWYT2e6efDhmUfEirAshSZ7pBOQn+MR1IZfWDvMrgtq/vbBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T18:34:53.222392Z"},"content_sha256":"a98eaa977e9573895add5ac30e24dc753700ba53ccfb7be550b1d2ec75b9e180","schema_version":"1.0","event_id":"sha256:a98eaa977e9573895add5ac30e24dc753700ba53ccfb7be550b1d2ec75b9e180"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CJ2PJC7PNMLA4M5SHYW7DURC2U/bundle.json","state_url":"https://pith.science/pith/CJ2PJC7PNMLA4M5SHYW7DURC2U/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CJ2PJC7PNMLA4M5SHYW7DURC2U/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":"2026-06-02T18:34:53Z","links":{"resolver":"https://pith.science/pith/CJ2PJC7PNMLA4M5SHYW7DURC2U","bundle":"https://pith.science/pith/CJ2PJC7PNMLA4M5SHYW7DURC2U/bundle.json","state":"https://pith.science/pith/CJ2PJC7PNMLA4M5SHYW7DURC2U/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CJ2PJC7PNMLA4M5SHYW7DURC2U/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:CJ2PJC7PNMLA4M5SHYW7DURC2U","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":"d9a4d102181472e460a19ec607b0331423bd1eea62e13d8549c39033faaa291b","cross_cats_sorted":["hep-lat","hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-11-26T20:55:49Z","title_canon_sha256":"90dc9cd5bf2c3d4585ceb0361e042eedb5dca0fe3e96abf5099b98e7df4c767f"},"schema_version":"1.0","source":{"id":"1211.6092","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.6092","created_at":"2026-05-18T03:20:09Z"},{"alias_kind":"arxiv_version","alias_value":"1211.6092v2","created_at":"2026-05-18T03:20:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.6092","created_at":"2026-05-18T03:20:09Z"},{"alias_kind":"pith_short_12","alias_value":"CJ2PJC7PNMLA","created_at":"2026-05-18T12:27:01Z"},{"alias_kind":"pith_short_16","alias_value":"CJ2PJC7PNMLA4M5S","created_at":"2026-05-18T12:27:01Z"},{"alias_kind":"pith_short_8","alias_value":"CJ2PJC7P","created_at":"2026-05-18T12:27:01Z"}],"graph_snapshots":[{"event_id":"sha256:a98eaa977e9573895add5ac30e24dc753700ba53ccfb7be550b1d2ec75b9e180","target":"graph","created_at":"2026-05-18T03:20:09Z","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 solve the Dyson-Schwinger equations of the ghost and gluon propagators of Landau gauge Yang-Mills theory together with that of the ghost-gluon vertex. The latter plays a central role in many truncation schemes for functional equations. By including it dynamically we can determine its influence on the propagators. We also suggest a new model for the three-gluon vertex motivated by lattice data which plays a crucial role to obtain stable solutions when the ghost-gluon vertex is included. We find that both vertices have a sizable quantitative impact on the mid-momentum regime and contribute to","authors_text":"Lorenz von Smekal, Markus Q. Huber","cross_cats":["hep-lat","hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-11-26T20:55:49Z","title":"On the influence of three-point functions on the propagators of Landau gauge Yang-Mills theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.6092","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:af9987b8327007a38371b043e806cc9b76280264470b8462856368554c0a63bd","target":"record","created_at":"2026-05-18T03:20:09Z","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":"d9a4d102181472e460a19ec607b0331423bd1eea62e13d8549c39033faaa291b","cross_cats_sorted":["hep-lat","hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-11-26T20:55:49Z","title_canon_sha256":"90dc9cd5bf2c3d4585ceb0361e042eedb5dca0fe3e96abf5099b98e7df4c767f"},"schema_version":"1.0","source":{"id":"1211.6092","kind":"arxiv","version":2}},"canonical_sha256":"1274f48bef6b160e33b23e2df1d222d51769240fc6d787789d886fbe1d9cd390","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1274f48bef6b160e33b23e2df1d222d51769240fc6d787789d886fbe1d9cd390","first_computed_at":"2026-05-18T03:20:09.472286Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:20:09.472286Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mEQL/b+ZGIxU1SF0czDOxD+bx2DcqAVj2O+afKs1I8PRAr9X8+zztMRRaMB6T0JwtGvRmGIzT2VvAzPES846DA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:20:09.472887Z","signed_message":"canonical_sha256_bytes"},"source_id":"1211.6092","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:af9987b8327007a38371b043e806cc9b76280264470b8462856368554c0a63bd","sha256:a98eaa977e9573895add5ac30e24dc753700ba53ccfb7be550b1d2ec75b9e180"],"state_sha256":"3530491dfe09a7c8915c747b96f6e2883a0a38764d2f8458e5b3b295f95b6d7a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2X9Lfq0z/BWBDFXjAEl7SkP+XEyr9sGCSyZnTvMMYZeP3KT18sJged/CiezNy6R6AnuCoiPtNzIWRjiOMLcNDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T18:34:53.224346Z","bundle_sha256":"9cd0e787e7445b9e48842da936a9f7d551ab6bf6e58a6c7293f881bf001e2c83"}}