{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:34W4UU6NDHZICSBIFMRTWJGYFC","short_pith_number":"pith:34W4UU6N","canonical_record":{"source":{"id":"hep-ph/0301107","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-01-15T16:11:19Z","cross_cats_sorted":[],"title_canon_sha256":"72dce52f0f1f0ebad81ea2707b5400baf18aa0e95196d4c1d3c5de7b48fd4d0d","abstract_canon_sha256":"afedad5d7a44907b521bb39b773de9ec7ba0a657e6e0cdc4c4be18eb282bf640"},"schema_version":"1.0"},"canonical_sha256":"df2dca53cd19f28148282b233b24d8289c16299824236f98a5e06bcec7e10fe1","source":{"kind":"arxiv","id":"hep-ph/0301107","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0301107","created_at":"2026-05-18T00:37:12Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0301107v1","created_at":"2026-05-18T00:37:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0301107","created_at":"2026-05-18T00:37:12Z"},{"alias_kind":"pith_short_12","alias_value":"34W4UU6NDHZI","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"34W4UU6NDHZICSBI","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"34W4UU6N","created_at":"2026-05-18T12:25:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:34W4UU6NDHZICSBIFMRTWJGYFC","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0301107","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-01-15T16:11:19Z","cross_cats_sorted":[],"title_canon_sha256":"72dce52f0f1f0ebad81ea2707b5400baf18aa0e95196d4c1d3c5de7b48fd4d0d","abstract_canon_sha256":"afedad5d7a44907b521bb39b773de9ec7ba0a657e6e0cdc4c4be18eb282bf640"},"schema_version":"1.0"},"canonical_sha256":"df2dca53cd19f28148282b233b24d8289c16299824236f98a5e06bcec7e10fe1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:12.031850Z","signature_b64":"K8okB6jTaatrVYA9HqlIcGMeKReaFL0V0m0S2wqpQlRGVbrgQO7pjifxvuyxHHhHsF6HUhRcoKusT/q8I2ivCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"df2dca53cd19f28148282b233b24d8289c16299824236f98a5e06bcec7e10fe1","last_reissued_at":"2026-05-18T00:37:12.031249Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:12.031249Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0301107","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":"2026-05-18T00:37:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sviQ8r94QcqEzGy8SWyZwzhwekmjCL8mnFV7S68rge/WQBGKIuPTT18XpVX++AhkYTo2Uz5kd0FvTc7vWYKcDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T23:25:42.196791Z"},"content_sha256":"b818c534b09102b4f4296c8758ef879261bff7514e24c5c1758dff41f86c1702","schema_version":"1.0","event_id":"sha256:b818c534b09102b4f4296c8758ef879261bff7514e24c5c1758dff41f86c1702"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:34W4UU6NDHZICSBIFMRTWJGYFC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Kugo-Ojima confinement criterion, Zwanziger-Gribov horizon condition, and infrared critical exponents in Landau gauge QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Christian S. Fischer, Lorenz von Smekal, Reinhard Alkofer","submitted_at":"2003-01-15T16:11:19Z","abstract_excerpt":"The Kugo-Ojima confinement criterion and its relation to the infrared behaviour of the gluon and ghost propagators in Landau gauge QCD are reviewed. The realization of this confinement criterion (which in Landau gauge relates to Zwanziger's horizon condition) results from quite general properties of the ghost Dyson-Schwinger equation. The numerical solutions for the gluon and ghost propagators obtained from a truncated set of Dyson-Schwinger equations provide an explicit example for the anticipated infrared behaviour. These results are in good agreement, also quantitatively, with corresponding"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0301107","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":"2026-05-18T00:37:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"08XM17Wg7M2kYqn7vyTd6WDPZ6cuINGPhqp/a2rhIbg8Mn8dAFkDdA3lPflyJ5ae4IWRouggt93khnIEV7M6Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T23:25:42.197528Z"},"content_sha256":"403590f88d02040d4ea5196b8f80fe17a69843f4572406e6911bf08ee01e5d0e","schema_version":"1.0","event_id":"sha256:403590f88d02040d4ea5196b8f80fe17a69843f4572406e6911bf08ee01e5d0e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/34W4UU6NDHZICSBIFMRTWJGYFC/bundle.json","state_url":"https://pith.science/pith/34W4UU6NDHZICSBIFMRTWJGYFC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/34W4UU6NDHZICSBIFMRTWJGYFC/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":"2026-05-31T23:25:42Z","links":{"resolver":"https://pith.science/pith/34W4UU6NDHZICSBIFMRTWJGYFC","bundle":"https://pith.science/pith/34W4UU6NDHZICSBIFMRTWJGYFC/bundle.json","state":"https://pith.science/pith/34W4UU6NDHZICSBIFMRTWJGYFC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/34W4UU6NDHZICSBIFMRTWJGYFC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:34W4UU6NDHZICSBIFMRTWJGYFC","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":"afedad5d7a44907b521bb39b773de9ec7ba0a657e6e0cdc4c4be18eb282bf640","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2003-01-15T16:11:19Z","title_canon_sha256":"72dce52f0f1f0ebad81ea2707b5400baf18aa0e95196d4c1d3c5de7b48fd4d0d"},"schema_version":"1.0","source":{"id":"hep-ph/0301107","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0301107","created_at":"2026-05-18T00:37:12Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0301107v1","created_at":"2026-05-18T00:37:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0301107","created_at":"2026-05-18T00:37:12Z"},{"alias_kind":"pith_short_12","alias_value":"34W4UU6NDHZI","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"34W4UU6NDHZICSBI","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"34W4UU6N","created_at":"2026-05-18T12:25:51Z"}],"graph_snapshots":[{"event_id":"sha256:403590f88d02040d4ea5196b8f80fe17a69843f4572406e6911bf08ee01e5d0e","target":"graph","created_at":"2026-05-18T00:37:12Z","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":"The Kugo-Ojima confinement criterion and its relation to the infrared behaviour of the gluon and ghost propagators in Landau gauge QCD are reviewed. The realization of this confinement criterion (which in Landau gauge relates to Zwanziger's horizon condition) results from quite general properties of the ghost Dyson-Schwinger equation. The numerical solutions for the gluon and ghost propagators obtained from a truncated set of Dyson-Schwinger equations provide an explicit example for the anticipated infrared behaviour. These results are in good agreement, also quantitatively, with corresponding","authors_text":"Christian S. Fischer, Lorenz von Smekal, Reinhard Alkofer","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2003-01-15T16:11:19Z","title":"Kugo-Ojima confinement criterion, Zwanziger-Gribov horizon condition, and infrared critical exponents in Landau gauge QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0301107","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:b818c534b09102b4f4296c8758ef879261bff7514e24c5c1758dff41f86c1702","target":"record","created_at":"2026-05-18T00:37:12Z","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":"afedad5d7a44907b521bb39b773de9ec7ba0a657e6e0cdc4c4be18eb282bf640","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2003-01-15T16:11:19Z","title_canon_sha256":"72dce52f0f1f0ebad81ea2707b5400baf18aa0e95196d4c1d3c5de7b48fd4d0d"},"schema_version":"1.0","source":{"id":"hep-ph/0301107","kind":"arxiv","version":1}},"canonical_sha256":"df2dca53cd19f28148282b233b24d8289c16299824236f98a5e06bcec7e10fe1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"df2dca53cd19f28148282b233b24d8289c16299824236f98a5e06bcec7e10fe1","first_computed_at":"2026-05-18T00:37:12.031249Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:37:12.031249Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"K8okB6jTaatrVYA9HqlIcGMeKReaFL0V0m0S2wqpQlRGVbrgQO7pjifxvuyxHHhHsF6HUhRcoKusT/q8I2ivCA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:37:12.031850Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0301107","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b818c534b09102b4f4296c8758ef879261bff7514e24c5c1758dff41f86c1702","sha256:403590f88d02040d4ea5196b8f80fe17a69843f4572406e6911bf08ee01e5d0e"],"state_sha256":"9a31616923caae1dae0a9c211c56d8247c380e1ac9c2f81f4d17755c8ff20f62"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ILOy97byTnxVCF+yB9FgWdZObwNG0H0dwquMv4oaJgSZt0uLxaAxRdDODeLvpc88wpSyKnWYt8k8GFbTNcKXBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T23:25:42.202046Z","bundle_sha256":"ef6d1a21e6b5f6d5b7bd9f4412611579341fafb9018a016adb65071f28e4715f"}}