{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2007:6ZS36CY5DRSA2FENDRTLFPB2OJ","short_pith_number":"pith:6ZS36CY5","canonical_record":{"source":{"id":"hep-lat/0702002","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2007-02-02T03:09:15Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"538eae1d716eb0a1212f614ee181e3787fdac6d5205ac22eec16cd53c4dc79e0","abstract_canon_sha256":"208398ae6696481c31e250abab879d171dcbdaed3d27bfdc585858f178e64a1e"},"schema_version":"1.0"},"canonical_sha256":"f665bf0b1d1c640d148d1c66b2bc3a726834b24d9fbac9665bbce006dd929520","source":{"kind":"arxiv","id":"hep-lat/0702002","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0702002","created_at":"2026-07-04T15:22:02Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0702002v1","created_at":"2026-07-04T15:22:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0702002","created_at":"2026-07-04T15:22:02Z"},{"alias_kind":"pith_short_12","alias_value":"6ZS36CY5DRSA","created_at":"2026-07-04T15:22:02Z"},{"alias_kind":"pith_short_16","alias_value":"6ZS36CY5DRSA2FEN","created_at":"2026-07-04T15:22:02Z"},{"alias_kind":"pith_short_8","alias_value":"6ZS36CY5","created_at":"2026-07-04T15:22:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2007:6ZS36CY5DRSA2FENDRTLFPB2OJ","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0702002","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2007-02-02T03:09:15Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"538eae1d716eb0a1212f614ee181e3787fdac6d5205ac22eec16cd53c4dc79e0","abstract_canon_sha256":"208398ae6696481c31e250abab879d171dcbdaed3d27bfdc585858f178e64a1e"},"schema_version":"1.0"},"canonical_sha256":"f665bf0b1d1c640d148d1c66b2bc3a726834b24d9fbac9665bbce006dd929520","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:22:02.940263Z","signature_b64":"YjiOJ90M3mwsRDBPUDdC68wY/e4Fcrg+j5P7Yt2Wts1Fw+QsPGu8sFKWiUJ+aKBMaH5V5Kp4ONj/ntcq4h2OCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f665bf0b1d1c640d148d1c66b2bc3a726834b24d9fbac9665bbce006dd929520","last_reissued_at":"2026-07-04T15:22:02.939908Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:22:02.939908Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0702002","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":"2026-07-04T15:22:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HZpjffQhnsGZ2/T7DcmAosw++WL7CNCdsNEwGCZtJtz0bw/psOWkBC1w8RCY61KFGBykXQ51rc2CLZByPGmyDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-28T16:15:47.430861Z"},"content_sha256":"9a3831b101c26ffe23b6603fd399ab74fe6e6b93b6b5784623ebd13d946b67d0","schema_version":"1.0","event_id":"sha256:9a3831b101c26ffe23b6603fd399ab74fe6e6b93b6b5784623ebd13d946b67d0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2007:6ZS36CY5DRSA2FENDRTLFPB2OJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Infrared behavior of the Faddeev-Popov operator in Coulomb gauge QCD","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"A. Nakamura, H. Toki, T. Saito, Y. Nakagawa","submitted_at":"2007-02-02T03:09:15Z","abstract_excerpt":"We calculate the eigenvalue distribution of the Faddeev-Popov operator in Coulomb gauge QCD using quenched SU(3) lattice simulation. In the confinement phase, the density of the low-lying eigenvalues increases with lattice volume, and the confinement criterion is satisfied. Moreover, even in the deconfinement phase, the behavior of the FP eigenvalue density is qualitatively the same as in the confinement phase. This is consistent with the fact that the color-Coulomb potential is not screened in the deconfined phase."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0702002","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/0702002/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T15:22:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"spC/galbc5771wjTp3kYS5d81V0VCFJaARqwdqj8ZTdkr8uwWFS7tnqdqLjLAw7g1VdwRqGwbLQXH4h9sA7kDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-28T16:15:47.431235Z"},"content_sha256":"2e673ad1f06ca74a5d2357b26706451e3276214133f288c1c35c8fb65efa36fd","schema_version":"1.0","event_id":"sha256:2e673ad1f06ca74a5d2357b26706451e3276214133f288c1c35c8fb65efa36fd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6ZS36CY5DRSA2FENDRTLFPB2OJ/bundle.json","state_url":"https://pith.science/pith/6ZS36CY5DRSA2FENDRTLFPB2OJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6ZS36CY5DRSA2FENDRTLFPB2OJ/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":"2026-07-28T16:15:47Z","links":{"resolver":"https://pith.science/pith/6ZS36CY5DRSA2FENDRTLFPB2OJ","bundle":"https://pith.science/pith/6ZS36CY5DRSA2FENDRTLFPB2OJ/bundle.json","state":"https://pith.science/pith/6ZS36CY5DRSA2FENDRTLFPB2OJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6ZS36CY5DRSA2FENDRTLFPB2OJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2007:6ZS36CY5DRSA2FENDRTLFPB2OJ","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":"208398ae6696481c31e250abab879d171dcbdaed3d27bfdc585858f178e64a1e","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-lat","submitted_at":"2007-02-02T03:09:15Z","title_canon_sha256":"538eae1d716eb0a1212f614ee181e3787fdac6d5205ac22eec16cd53c4dc79e0"},"schema_version":"1.0","source":{"id":"hep-lat/0702002","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0702002","created_at":"2026-07-04T15:22:02Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0702002v1","created_at":"2026-07-04T15:22:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0702002","created_at":"2026-07-04T15:22:02Z"},{"alias_kind":"pith_short_12","alias_value":"6ZS36CY5DRSA","created_at":"2026-07-04T15:22:02Z"},{"alias_kind":"pith_short_16","alias_value":"6ZS36CY5DRSA2FEN","created_at":"2026-07-04T15:22:02Z"},{"alias_kind":"pith_short_8","alias_value":"6ZS36CY5","created_at":"2026-07-04T15:22:02Z"}],"graph_snapshots":[{"event_id":"sha256:2e673ad1f06ca74a5d2357b26706451e3276214133f288c1c35c8fb65efa36fd","target":"graph","created_at":"2026-07-04T15:22:02Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-lat/0702002/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We calculate the eigenvalue distribution of the Faddeev-Popov operator in Coulomb gauge QCD using quenched SU(3) lattice simulation. In the confinement phase, the density of the low-lying eigenvalues increases with lattice volume, and the confinement criterion is satisfied. Moreover, even in the deconfinement phase, the behavior of the FP eigenvalue density is qualitatively the same as in the confinement phase. This is consistent with the fact that the color-Coulomb potential is not screened in the deconfined phase.","authors_text":"A. Nakamura, H. Toki, T. Saito, Y. Nakagawa","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2007-02-02T03:09:15Z","title":"Infrared behavior of the Faddeev-Popov operator in Coulomb gauge QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0702002","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":"sha256:9a3831b101c26ffe23b6603fd399ab74fe6e6b93b6b5784623ebd13d946b67d0","target":"record","created_at":"2026-07-04T15:22:02Z","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":"208398ae6696481c31e250abab879d171dcbdaed3d27bfdc585858f178e64a1e","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-lat","submitted_at":"2007-02-02T03:09:15Z","title_canon_sha256":"538eae1d716eb0a1212f614ee181e3787fdac6d5205ac22eec16cd53c4dc79e0"},"schema_version":"1.0","source":{"id":"hep-lat/0702002","kind":"arxiv","version":1}},"canonical_sha256":"f665bf0b1d1c640d148d1c66b2bc3a726834b24d9fbac9665bbce006dd929520","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f665bf0b1d1c640d148d1c66b2bc3a726834b24d9fbac9665bbce006dd929520","first_computed_at":"2026-07-04T15:22:02.939908Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:22:02.939908Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"YjiOJ90M3mwsRDBPUDdC68wY/e4Fcrg+j5P7Yt2Wts1Fw+QsPGu8sFKWiUJ+aKBMaH5V5Kp4ONj/ntcq4h2OCA==","signature_status":"signed_v1","signed_at":"2026-07-04T15:22:02.940263Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0702002","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9a3831b101c26ffe23b6603fd399ab74fe6e6b93b6b5784623ebd13d946b67d0","sha256:2e673ad1f06ca74a5d2357b26706451e3276214133f288c1c35c8fb65efa36fd"],"state_sha256":"4f606705c69987e15e4fdc097b76c3de7a3635ab922f5b2817cf71460228d172"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zlmALkFQ28GnHG38aBs5QGrD5QBgms6w62nx8Yc2xFOZtaWvs6JiCZYJn13VVu53gRGSdoZ3OHtb+9twEhJ0Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-28T16:15:47.433699Z","bundle_sha256":"beea70374cceba1b5aebe02eec8a083487f3e05abecf2e46e2bd4bce8711e7c9"}}