{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2001:DUW3GU6ITZPOIN2UHV6JKOE634","short_pith_number":"pith:DUW3GU6I","canonical_record":{"source":{"id":"hep-lat/0105006","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2001-05-07T02:31:45Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"7e083aaa455cc3e727ab03f935f15314f3264d788718a23f31ba875700eaab4c","abstract_canon_sha256":"87666543671679a0a2a56121353876a40ffdc234be5c066c7acc5851381b4fdf"},"schema_version":"1.0"},"canonical_sha256":"1d2db353c89e5ee437543d7c95389edf1d11735314733ddb0f4928dcb700bdca","source":{"kind":"arxiv","id":"hep-lat/0105006","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0105006","created_at":"2026-07-04T16:27:08Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0105006v1","created_at":"2026-07-04T16:27:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0105006","created_at":"2026-07-04T16:27:08Z"},{"alias_kind":"pith_short_12","alias_value":"DUW3GU6ITZPO","created_at":"2026-07-04T16:27:08Z"},{"alias_kind":"pith_short_16","alias_value":"DUW3GU6ITZPOIN2U","created_at":"2026-07-04T16:27:08Z"},{"alias_kind":"pith_short_8","alias_value":"DUW3GU6I","created_at":"2026-07-04T16:27:08Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2001:DUW3GU6ITZPOIN2UHV6JKOE634","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0105006","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2001-05-07T02:31:45Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"7e083aaa455cc3e727ab03f935f15314f3264d788718a23f31ba875700eaab4c","abstract_canon_sha256":"87666543671679a0a2a56121353876a40ffdc234be5c066c7acc5851381b4fdf"},"schema_version":"1.0"},"canonical_sha256":"1d2db353c89e5ee437543d7c95389edf1d11735314733ddb0f4928dcb700bdca","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:08.024145Z","signature_b64":"09lILLQsl4ksC0Ge+0gUvSLF44964CkDA3Wv7Fb2OumEsCjh2d+ENcgstfJYJjh0xQ83Qjj6cbVMmLL3haXzAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1d2db353c89e5ee437543d7c95389edf1d11735314733ddb0f4928dcb700bdca","last_reissued_at":"2026-07-04T16:27:08.023792Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:08.023792Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0105006","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":"2026-07-04T16:27:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"G7wA4TQaJuKCE1cgYaXaRGfMq/NKlwnCy97/1jeqhfOIJ2yDYjdTHtKSS2JvKwAngtEpe1yOUrh2q+s7oXXHBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T13:58:55.361050Z"},"content_sha256":"2ceab6227a123d22f55a34af23123b439a6471c5008e9b0611fa46c9e54fee49","schema_version":"1.0","event_id":"sha256:2ceab6227a123d22f55a34af23123b439a6471c5008e9b0611fa46c9e54fee49"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2001:DUW3GU6ITZPOIN2UHV6JKOE634","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Chirality Correlation within Dirac Eigenvectors from Domain Wall Fermions","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-lat","authors_text":"C. Cristian, C. Dawson, G. Liu, L. Wu, N. Christ, R. Mawhinney, T. Blum, X. Liao, Y. Zhestkov","submitted_at":"2001-05-07T02:31:45Z","abstract_excerpt":"In the dilute instanton gas model of the QCD vacuum, one expects a strong spatial correlation between chirality and the maxima of the Dirac eigenvectors with small eigenvalues. Following Horvath, {\\it et al.} we examine this question using lattice gauge theory within the quenched approximation. We extend the work of those authors by using weaker coupling, $\\beta=6.0$, larger lattices, $16^4$, and an improved fermion formulation, domain wall fermions. In contrast with this earlier work, we find a striking correlation between the magnitude of the chirality density, $|\\psi^\\dagger(x)\\gamma^5\\psi("},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0105006","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/0105006/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":"2026-07-04T16:27:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HL6ijwkiTycb4pQzhj/bhfIJfFqG4YBk1n71bw1bs3X0lYxaSOJwMkzYtp/xrjpxUlHNGX744WFdME/6+vh9AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T13:58:55.361693Z"},"content_sha256":"2ede4b70d4006ab4fa07b0f9965be02fc9d43725883d2ccef4ccf32bc602b06a","schema_version":"1.0","event_id":"sha256:2ede4b70d4006ab4fa07b0f9965be02fc9d43725883d2ccef4ccf32bc602b06a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DUW3GU6ITZPOIN2UHV6JKOE634/bundle.json","state_url":"https://pith.science/pith/DUW3GU6ITZPOIN2UHV6JKOE634/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DUW3GU6ITZPOIN2UHV6JKOE634/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":"2026-08-15T13:58:55Z","links":{"resolver":"https://pith.science/pith/DUW3GU6ITZPOIN2UHV6JKOE634","bundle":"https://pith.science/pith/DUW3GU6ITZPOIN2UHV6JKOE634/bundle.json","state":"https://pith.science/pith/DUW3GU6ITZPOIN2UHV6JKOE634/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DUW3GU6ITZPOIN2UHV6JKOE634/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2001:DUW3GU6ITZPOIN2UHV6JKOE634","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":"87666543671679a0a2a56121353876a40ffdc234be5c066c7acc5851381b4fdf","cross_cats_sorted":["hep-th"],"license":"","primary_cat":"hep-lat","submitted_at":"2001-05-07T02:31:45Z","title_canon_sha256":"7e083aaa455cc3e727ab03f935f15314f3264d788718a23f31ba875700eaab4c"},"schema_version":"1.0","source":{"id":"hep-lat/0105006","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0105006","created_at":"2026-07-04T16:27:08Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0105006v1","created_at":"2026-07-04T16:27:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0105006","created_at":"2026-07-04T16:27:08Z"},{"alias_kind":"pith_short_12","alias_value":"DUW3GU6ITZPO","created_at":"2026-07-04T16:27:08Z"},{"alias_kind":"pith_short_16","alias_value":"DUW3GU6ITZPOIN2U","created_at":"2026-07-04T16:27:08Z"},{"alias_kind":"pith_short_8","alias_value":"DUW3GU6I","created_at":"2026-07-04T16:27:08Z"}],"graph_snapshots":[{"event_id":"sha256:2ede4b70d4006ab4fa07b0f9965be02fc9d43725883d2ccef4ccf32bc602b06a","target":"graph","created_at":"2026-07-04T16:27:08Z","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/0105006/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In the dilute instanton gas model of the QCD vacuum, one expects a strong spatial correlation between chirality and the maxima of the Dirac eigenvectors with small eigenvalues. Following Horvath, {\\it et al.} we examine this question using lattice gauge theory within the quenched approximation. We extend the work of those authors by using weaker coupling, $\\beta=6.0$, larger lattices, $16^4$, and an improved fermion formulation, domain wall fermions. In contrast with this earlier work, we find a striking correlation between the magnitude of the chirality density, $|\\psi^\\dagger(x)\\gamma^5\\psi(","authors_text":"C. Cristian, C. Dawson, G. Liu, L. Wu, N. Christ, R. Mawhinney, T. Blum, X. Liao, Y. Zhestkov","cross_cats":["hep-th"],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2001-05-07T02:31:45Z","title":"Chirality Correlation within Dirac Eigenvectors from Domain Wall Fermions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0105006","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":"sha256:2ceab6227a123d22f55a34af23123b439a6471c5008e9b0611fa46c9e54fee49","target":"record","created_at":"2026-07-04T16:27:08Z","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":"87666543671679a0a2a56121353876a40ffdc234be5c066c7acc5851381b4fdf","cross_cats_sorted":["hep-th"],"license":"","primary_cat":"hep-lat","submitted_at":"2001-05-07T02:31:45Z","title_canon_sha256":"7e083aaa455cc3e727ab03f935f15314f3264d788718a23f31ba875700eaab4c"},"schema_version":"1.0","source":{"id":"hep-lat/0105006","kind":"arxiv","version":1}},"canonical_sha256":"1d2db353c89e5ee437543d7c95389edf1d11735314733ddb0f4928dcb700bdca","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1d2db353c89e5ee437543d7c95389edf1d11735314733ddb0f4928dcb700bdca","first_computed_at":"2026-07-04T16:27:08.023792Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:27:08.023792Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"09lILLQsl4ksC0Ge+0gUvSLF44964CkDA3Wv7Fb2OumEsCjh2d+ENcgstfJYJjh0xQ83Qjj6cbVMmLL3haXzAw==","signature_status":"signed_v1","signed_at":"2026-07-04T16:27:08.024145Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0105006","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2ceab6227a123d22f55a34af23123b439a6471c5008e9b0611fa46c9e54fee49","sha256:2ede4b70d4006ab4fa07b0f9965be02fc9d43725883d2ccef4ccf32bc602b06a"],"state_sha256":"394c3dcb9b2de66a0ce22614ba94bf91f19510e9d2124ca7de46f5352433b2ba"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"utMzr3Cv8oowgqyW0eiC4woPBTXcjwUzo70IbHKSS0LhT9JeEcFKNsfWmOpca74AeHcFk639slUB1VHisfodCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-15T13:58:55.365661Z","bundle_sha256":"76acde7f1caa5a9d57a8fdb2572f3edf89fb734553a7c2766d32a725bc6bd324"}}