{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:3YSKCD4RP3O3TTT37MQ7KLTH72","short_pith_number":"pith:3YSKCD4R","canonical_record":{"source":{"id":"hep-lat/0203019","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2002-03-18T06:12:29Z","cross_cats_sorted":[],"title_canon_sha256":"c7e0064ffd353f2afc49eedd07939069c6f15f75a753dfbf8c0491d609970f8b","abstract_canon_sha256":"d0687ff676c40a00006251b4110af7e695ad52c8789058d31914721af905b7ef"},"schema_version":"1.0"},"canonical_sha256":"de24a10f917eddb9ce7bfb21f52e67feb62f2b9493e7f1884954f0a6ba40dc4e","source":{"kind":"arxiv","id":"hep-lat/0203019","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0203019","created_at":"2026-05-18T01:06:39Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0203019v1","created_at":"2026-05-18T01:06:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0203019","created_at":"2026-05-18T01:06:39Z"},{"alias_kind":"pith_short_12","alias_value":"3YSKCD4RP3O3","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"3YSKCD4RP3O3TTT3","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"3YSKCD4R","created_at":"2026-05-18T12:25:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:3YSKCD4RP3O3TTT37MQ7KLTH72","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0203019","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2002-03-18T06:12:29Z","cross_cats_sorted":[],"title_canon_sha256":"c7e0064ffd353f2afc49eedd07939069c6f15f75a753dfbf8c0491d609970f8b","abstract_canon_sha256":"d0687ff676c40a00006251b4110af7e695ad52c8789058d31914721af905b7ef"},"schema_version":"1.0"},"canonical_sha256":"de24a10f917eddb9ce7bfb21f52e67feb62f2b9493e7f1884954f0a6ba40dc4e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:39.229512Z","signature_b64":"6BAufxp1YN6ywBzsVZurKwW3yCg9FXmXVIz6hJLQ20MBU+yvTek1yDr/f4EGBsLuAZ0181oinyn3mNanLc50Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"de24a10f917eddb9ce7bfb21f52e67feb62f2b9493e7f1884954f0a6ba40dc4e","last_reissued_at":"2026-05-18T01:06:39.228805Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:39.228805Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0203019","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":"2026-05-18T01:06:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5Ts8XUZSnDIQYU75QZYYStDHRZ/510IVDhMlquTieKVq5VFX/hLHdnCpxNxGsrpxZ6WrCYaISnPUXoh0aBQWCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T06:45:57.251483Z"},"content_sha256":"7dccf4c8d9f8e984554469f50517e40b4888ce8c44e5a83c344fbf5e44dbfbe5","schema_version":"1.0","event_id":"sha256:7dccf4c8d9f8e984554469f50517e40b4888ce8c44e5a83c344fbf5e44dbfbe5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:3YSKCD4RP3O3TTT37MQ7KLTH72","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Ginsparg-Wilson Relation and Lattice Chiral Symmetry in Fermionic Interacting Theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Hiroto So, Naoya Ukita, Yuji Igarashi","submitted_at":"2002-03-18T06:12:29Z","abstract_excerpt":"We derive Ginsparg-Wilson relation for a lattice chiral symmetry in theories with self-interacting fermions. Auxiliary scalar and pseudo-scalar fields are introduced on a coarse lattice to give an effective description of the fermionic interactions. We obtain particular solutions to the Ginsparg-Wilson relation and other\n Ward-Takahashi identities in a closed form. These non-perturbative solutions can be used to construct a chiral invariant action and an invariant path-integral measure on the coarse lattice. The resulting partition function exhibits the exact chiral symmetry in the fermionic s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0203019","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":"2026-05-18T01:06:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kVvU4lkow7VBX18CoBsRugqDggZR/8HRPUk0L2f3vrrvP6/vyoO7DzaIzZLx1xG5V5Rj7So1XtrVoLiFHn/3AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T06:45:57.251834Z"},"content_sha256":"5be04a5552dd6bd173e831cfe2ad6504cfa551c8f57bb79185809d45881aff34","schema_version":"1.0","event_id":"sha256:5be04a5552dd6bd173e831cfe2ad6504cfa551c8f57bb79185809d45881aff34"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3YSKCD4RP3O3TTT37MQ7KLTH72/bundle.json","state_url":"https://pith.science/pith/3YSKCD4RP3O3TTT37MQ7KLTH72/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3YSKCD4RP3O3TTT37MQ7KLTH72/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":"2026-05-28T06:45:57Z","links":{"resolver":"https://pith.science/pith/3YSKCD4RP3O3TTT37MQ7KLTH72","bundle":"https://pith.science/pith/3YSKCD4RP3O3TTT37MQ7KLTH72/bundle.json","state":"https://pith.science/pith/3YSKCD4RP3O3TTT37MQ7KLTH72/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3YSKCD4RP3O3TTT37MQ7KLTH72/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:3YSKCD4RP3O3TTT37MQ7KLTH72","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":"d0687ff676c40a00006251b4110af7e695ad52c8789058d31914721af905b7ef","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2002-03-18T06:12:29Z","title_canon_sha256":"c7e0064ffd353f2afc49eedd07939069c6f15f75a753dfbf8c0491d609970f8b"},"schema_version":"1.0","source":{"id":"hep-lat/0203019","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0203019","created_at":"2026-05-18T01:06:39Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0203019v1","created_at":"2026-05-18T01:06:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0203019","created_at":"2026-05-18T01:06:39Z"},{"alias_kind":"pith_short_12","alias_value":"3YSKCD4RP3O3","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"3YSKCD4RP3O3TTT3","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"3YSKCD4R","created_at":"2026-05-18T12:25:50Z"}],"graph_snapshots":[{"event_id":"sha256:5be04a5552dd6bd173e831cfe2ad6504cfa551c8f57bb79185809d45881aff34","target":"graph","created_at":"2026-05-18T01:06:39Z","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 derive Ginsparg-Wilson relation for a lattice chiral symmetry in theories with self-interacting fermions. Auxiliary scalar and pseudo-scalar fields are introduced on a coarse lattice to give an effective description of the fermionic interactions. We obtain particular solutions to the Ginsparg-Wilson relation and other\n Ward-Takahashi identities in a closed form. These non-perturbative solutions can be used to construct a chiral invariant action and an invariant path-integral measure on the coarse lattice. The resulting partition function exhibits the exact chiral symmetry in the fermionic s","authors_text":"Hiroto So, Naoya Ukita, Yuji Igarashi","cross_cats":[],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2002-03-18T06:12:29Z","title":"Ginsparg-Wilson Relation and Lattice Chiral Symmetry in Fermionic Interacting Theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0203019","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":"sha256:7dccf4c8d9f8e984554469f50517e40b4888ce8c44e5a83c344fbf5e44dbfbe5","target":"record","created_at":"2026-05-18T01:06:39Z","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":"d0687ff676c40a00006251b4110af7e695ad52c8789058d31914721af905b7ef","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2002-03-18T06:12:29Z","title_canon_sha256":"c7e0064ffd353f2afc49eedd07939069c6f15f75a753dfbf8c0491d609970f8b"},"schema_version":"1.0","source":{"id":"hep-lat/0203019","kind":"arxiv","version":1}},"canonical_sha256":"de24a10f917eddb9ce7bfb21f52e67feb62f2b9493e7f1884954f0a6ba40dc4e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"de24a10f917eddb9ce7bfb21f52e67feb62f2b9493e7f1884954f0a6ba40dc4e","first_computed_at":"2026-05-18T01:06:39.228805Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:06:39.228805Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6BAufxp1YN6ywBzsVZurKwW3yCg9FXmXVIz6hJLQ20MBU+yvTek1yDr/f4EGBsLuAZ0181oinyn3mNanLc50Cw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:06:39.229512Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0203019","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7dccf4c8d9f8e984554469f50517e40b4888ce8c44e5a83c344fbf5e44dbfbe5","sha256:5be04a5552dd6bd173e831cfe2ad6504cfa551c8f57bb79185809d45881aff34"],"state_sha256":"9b64a78464154f8441a7be8b64875b3ee2be755798b8c3092e0a0318ad2c1c49"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"drcRaOufV4CKoG5h4ZV+9PXNG1kbalZBeQ/NGjBCPqMMpXQvdp7Xnr4/ch8r7YkgnXTt5QTydxnGsvZiVkKeDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T06:45:57.254036Z","bundle_sha256":"12b18d8221ed662a142054f4a6d641a2d03e64220003279c2e90a290ad03c42a"}}