{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:6S6JWOKKXIIJC423GVVLE36TB3","short_pith_number":"pith:6S6JWOKK","canonical_record":{"source":{"id":"hep-lat/0603029","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2006-03-30T11:58:48Z","cross_cats_sorted":[],"title_canon_sha256":"f80f7ac36be72b6d0cae3720211d080a8ecc04bdc7697748c8a247c44cbb25f8","abstract_canon_sha256":"90eeb246abc08e270feda6063fad5a05bb3e59cf9207d5d9ea3ffbf320a2dfdd"},"schema_version":"1.0"},"canonical_sha256":"f4bc9b394aba1091735b356ab26fd30ef1b8bdc745dcef41b0e60db559515860","source":{"kind":"arxiv","id":"hep-lat/0603029","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0603029","created_at":"2026-07-04T17:01:37Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0603029v1","created_at":"2026-07-04T17:01:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0603029","created_at":"2026-07-04T17:01:37Z"},{"alias_kind":"pith_short_12","alias_value":"6S6JWOKKXIIJ","created_at":"2026-07-04T17:01:37Z"},{"alias_kind":"pith_short_16","alias_value":"6S6JWOKKXIIJC423","created_at":"2026-07-04T17:01:37Z"},{"alias_kind":"pith_short_8","alias_value":"6S6JWOKK","created_at":"2026-07-04T17:01:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:6S6JWOKKXIIJC423GVVLE36TB3","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0603029","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2006-03-30T11:58:48Z","cross_cats_sorted":[],"title_canon_sha256":"f80f7ac36be72b6d0cae3720211d080a8ecc04bdc7697748c8a247c44cbb25f8","abstract_canon_sha256":"90eeb246abc08e270feda6063fad5a05bb3e59cf9207d5d9ea3ffbf320a2dfdd"},"schema_version":"1.0"},"canonical_sha256":"f4bc9b394aba1091735b356ab26fd30ef1b8bdc745dcef41b0e60db559515860","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:01:37.581979Z","signature_b64":"vpmaI2+/OYzbT3Cz159xBXPygUlDPvh//XrkP81JKy7i2s0+mxCM9i6qAnG3Vl9CnyvdZu/BuvV125iHu4ZUAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f4bc9b394aba1091735b356ab26fd30ef1b8bdc745dcef41b0e60db559515860","last_reissued_at":"2026-07-04T17:01:37.581608Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:01:37.581608Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0603029","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":"2026-07-04T17:01:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZJpROauSe2CBj0hI+q0+watbMOPdEuo6L5rnA23Y6J0rwha5B1KruMXmxDUqxTfSUwEXMiMWFJr2YhpLtd9XBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T21:59:21.966876Z"},"content_sha256":"a2397fbee2884a008985771cd6994bc5fd056c8af834062245db5ffd9e9584bd","schema_version":"1.0","event_id":"sha256:a2397fbee2884a008985771cd6994bc5fd056c8af834062245db5ffd9e9584bd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:6S6JWOKKXIIJC423GVVLE36TB3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The Schr\\\"odinger functional in lattice QCD with exact chiral symmetry","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Martin L\\\"uscher","submitted_at":"2006-03-30T11:58:48Z","abstract_excerpt":"Similarly to the interaction lagrangian, the possible boundary conditions in quantum field theories on space-time manifolds with boundaries are strongly constrained by the symmetry and scaling properties of the theory. Based on this general insight, a lattice formulation of the QCD Schr\\\"odinger functional is proposed for the case where the lattice Dirac operator in the bulk of the lattice coincides with the Neuberger--Dirac operator. The construction satisfies all basic requirements (locality, symmetries, hermiticity) and is suitable for numerical simulations."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0603029","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/0603029/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":"2026-07-04T17:01:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GK6kfdIrvu+El4Fwg80lDSiW2n5vuanImI479eZ/L8rcFbQAbuSxEqGg0EkZJWkvj/2zz0+MKuvAk09QmOb7Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T21:59:21.967401Z"},"content_sha256":"01964c69fb922c3a13cb9fb4acbbd5acadfd302a020148776a4998b758a63915","schema_version":"1.0","event_id":"sha256:01964c69fb922c3a13cb9fb4acbbd5acadfd302a020148776a4998b758a63915"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6S6JWOKKXIIJC423GVVLE36TB3/bundle.json","state_url":"https://pith.science/pith/6S6JWOKKXIIJC423GVVLE36TB3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6S6JWOKKXIIJC423GVVLE36TB3/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":"2026-08-13T21:59:22Z","links":{"resolver":"https://pith.science/pith/6S6JWOKKXIIJC423GVVLE36TB3","bundle":"https://pith.science/pith/6S6JWOKKXIIJC423GVVLE36TB3/bundle.json","state":"https://pith.science/pith/6S6JWOKKXIIJC423GVVLE36TB3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6S6JWOKKXIIJC423GVVLE36TB3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:6S6JWOKKXIIJC423GVVLE36TB3","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":"90eeb246abc08e270feda6063fad5a05bb3e59cf9207d5d9ea3ffbf320a2dfdd","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2006-03-30T11:58:48Z","title_canon_sha256":"f80f7ac36be72b6d0cae3720211d080a8ecc04bdc7697748c8a247c44cbb25f8"},"schema_version":"1.0","source":{"id":"hep-lat/0603029","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0603029","created_at":"2026-07-04T17:01:37Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0603029v1","created_at":"2026-07-04T17:01:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0603029","created_at":"2026-07-04T17:01:37Z"},{"alias_kind":"pith_short_12","alias_value":"6S6JWOKKXIIJ","created_at":"2026-07-04T17:01:37Z"},{"alias_kind":"pith_short_16","alias_value":"6S6JWOKKXIIJC423","created_at":"2026-07-04T17:01:37Z"},{"alias_kind":"pith_short_8","alias_value":"6S6JWOKK","created_at":"2026-07-04T17:01:37Z"}],"graph_snapshots":[{"event_id":"sha256:01964c69fb922c3a13cb9fb4acbbd5acadfd302a020148776a4998b758a63915","target":"graph","created_at":"2026-07-04T17:01:37Z","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/0603029/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Similarly to the interaction lagrangian, the possible boundary conditions in quantum field theories on space-time manifolds with boundaries are strongly constrained by the symmetry and scaling properties of the theory. Based on this general insight, a lattice formulation of the QCD Schr\\\"odinger functional is proposed for the case where the lattice Dirac operator in the bulk of the lattice coincides with the Neuberger--Dirac operator. The construction satisfies all basic requirements (locality, symmetries, hermiticity) and is suitable for numerical simulations.","authors_text":"Martin L\\\"uscher","cross_cats":[],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2006-03-30T11:58:48Z","title":"The Schr\\\"odinger functional in lattice QCD with exact chiral symmetry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0603029","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:a2397fbee2884a008985771cd6994bc5fd056c8af834062245db5ffd9e9584bd","target":"record","created_at":"2026-07-04T17:01:37Z","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":"90eeb246abc08e270feda6063fad5a05bb3e59cf9207d5d9ea3ffbf320a2dfdd","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2006-03-30T11:58:48Z","title_canon_sha256":"f80f7ac36be72b6d0cae3720211d080a8ecc04bdc7697748c8a247c44cbb25f8"},"schema_version":"1.0","source":{"id":"hep-lat/0603029","kind":"arxiv","version":1}},"canonical_sha256":"f4bc9b394aba1091735b356ab26fd30ef1b8bdc745dcef41b0e60db559515860","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f4bc9b394aba1091735b356ab26fd30ef1b8bdc745dcef41b0e60db559515860","first_computed_at":"2026-07-04T17:01:37.581608Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T17:01:37.581608Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vpmaI2+/OYzbT3Cz159xBXPygUlDPvh//XrkP81JKy7i2s0+mxCM9i6qAnG3Vl9CnyvdZu/BuvV125iHu4ZUAw==","signature_status":"signed_v1","signed_at":"2026-07-04T17:01:37.581979Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0603029","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a2397fbee2884a008985771cd6994bc5fd056c8af834062245db5ffd9e9584bd","sha256:01964c69fb922c3a13cb9fb4acbbd5acadfd302a020148776a4998b758a63915"],"state_sha256":"1b6a0ab78fd48c951d1c9e971464d49d0253663f574abb47b1bb34d9ca5e0045"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zIxgxRoVX+RLkhJVlTjFjCZoN/zBB6F5++wCSO6g0QhX0iNPug6bP3ZuEUyFARPpPfL8MnzgYyQLDQp5wIMvCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-13T21:59:22.006142Z","bundle_sha256":"5d3238de94158426c8398972cd5586ef3d9eab56262accae5d40155e85a7c794"}}