{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1995:43IFALKWCMXJ5TOPMVTXUPKRVL","short_pith_number":"pith:43IFALKW","canonical_record":{"source":{"id":"hep-lat/9509079","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1995-09-25T13:54:33Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"ae531faca9fefd4bc5b044ab7da00cc2e1909fb5d10bd7574a9b838240afd20c","abstract_canon_sha256":"e6245a77a0b39d97df7a152ab8124ab24ac59a95c8fdea02007c4db3750fc4a3"},"schema_version":"1.0"},"canonical_sha256":"e6d0502d56132e9ecdcf65677a3d51aadae655b0c2c1cc3b7496d40cf2c1c862","source":{"kind":"arxiv","id":"hep-lat/9509079","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9509079","created_at":"2026-07-04T15:29:30Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9509079v1","created_at":"2026-07-04T15:29:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9509079","created_at":"2026-07-04T15:29:30Z"},{"alias_kind":"pith_short_12","alias_value":"43IFALKWCMXJ","created_at":"2026-07-04T15:29:30Z"},{"alias_kind":"pith_short_16","alias_value":"43IFALKWCMXJ5TOP","created_at":"2026-07-04T15:29:30Z"},{"alias_kind":"pith_short_8","alias_value":"43IFALKW","created_at":"2026-07-04T15:29:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1995:43IFALKWCMXJ5TOPMVTXUPKRVL","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/9509079","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1995-09-25T13:54:33Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"ae531faca9fefd4bc5b044ab7da00cc2e1909fb5d10bd7574a9b838240afd20c","abstract_canon_sha256":"e6245a77a0b39d97df7a152ab8124ab24ac59a95c8fdea02007c4db3750fc4a3"},"schema_version":"1.0"},"canonical_sha256":"e6d0502d56132e9ecdcf65677a3d51aadae655b0c2c1cc3b7496d40cf2c1c862","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:29:30.543567Z","signature_b64":"llazbUWM0BJ2h5dRmiKVRiIWEvf+Dq+FrmEyxnPPAFBM8MP1oDfbQOXeGgjxnbuCH0RX7mF5YMoCnRYTK9rSBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e6d0502d56132e9ecdcf65677a3d51aadae655b0c2c1cc3b7496d40cf2c1c862","last_reissued_at":"2026-07-04T15:29:30.543151Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:29:30.543151Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/9509079","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":"2026-07-04T15:29:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IWzn6yX9dkALva9OheeSMi7n3P4btNtSiyiDf/qkXGVrTAdT2AbVvbzJr86PrlJZ9XB+vJEh9LECELjZ9a5TAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T20:20:44.445166Z"},"content_sha256":"b255933750d458b2deaa0fd139763a967a47e03ff5074d1b0f8655e14cee8b80","schema_version":"1.0","event_id":"sha256:b255933750d458b2deaa0fd139763a967a47e03ff5074d1b0f8655e14cee8b80"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1995:43IFALKWCMXJ5TOPMVTXUPKRVL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A Lattice Evaluation of the Deep-Inelastic Structure Functions of the Nucleon","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"A. Schiller, E.-M. Ilgenfritz, G. Schierholz, H. Oelrich, H. Perlt, M. G\\\"ockeler, P. Rakow, R. Horsley","submitted_at":"1995-09-25T13:54:33Z","abstract_excerpt":"The lower moments of the unpolarized and polarized deep-inelastic structure functions of the nucleon are calculated on the lattice. The calculation is done with Wilson fermions and for three values of the hopping parameter $\\kappa$, so that we can perform the extrapolation to the chiral limit. Particular emphasis is put on the renormalization of lattice operators. The renormalization constants, which lead us from lattice to continuum operators, are computed perturbatively to one loop order as well as non-perturbatively."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9509079","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/9509079/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":"2026-07-04T15:29:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4Q7Zp1kVCEGyFNwfeGEvYXLhTeHNg1b3cWNzOQGGnt0ubuYcD9LKfRv2iq1p0o4c9oIqGmlTqgbJqI+4wTclCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T20:20:44.445978Z"},"content_sha256":"9d6eafe0fe9f297c4933b1e07de1fc14ddfbffdbd44049d52800fde13d092a25","schema_version":"1.0","event_id":"sha256:9d6eafe0fe9f297c4933b1e07de1fc14ddfbffdbd44049d52800fde13d092a25"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/43IFALKWCMXJ5TOPMVTXUPKRVL/bundle.json","state_url":"https://pith.science/pith/43IFALKWCMXJ5TOPMVTXUPKRVL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/43IFALKWCMXJ5TOPMVTXUPKRVL/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":"2026-08-06T20:20:44Z","links":{"resolver":"https://pith.science/pith/43IFALKWCMXJ5TOPMVTXUPKRVL","bundle":"https://pith.science/pith/43IFALKWCMXJ5TOPMVTXUPKRVL/bundle.json","state":"https://pith.science/pith/43IFALKWCMXJ5TOPMVTXUPKRVL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/43IFALKWCMXJ5TOPMVTXUPKRVL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1995:43IFALKWCMXJ5TOPMVTXUPKRVL","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":"e6245a77a0b39d97df7a152ab8124ab24ac59a95c8fdea02007c4db3750fc4a3","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-lat","submitted_at":"1995-09-25T13:54:33Z","title_canon_sha256":"ae531faca9fefd4bc5b044ab7da00cc2e1909fb5d10bd7574a9b838240afd20c"},"schema_version":"1.0","source":{"id":"hep-lat/9509079","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9509079","created_at":"2026-07-04T15:29:30Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9509079v1","created_at":"2026-07-04T15:29:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9509079","created_at":"2026-07-04T15:29:30Z"},{"alias_kind":"pith_short_12","alias_value":"43IFALKWCMXJ","created_at":"2026-07-04T15:29:30Z"},{"alias_kind":"pith_short_16","alias_value":"43IFALKWCMXJ5TOP","created_at":"2026-07-04T15:29:30Z"},{"alias_kind":"pith_short_8","alias_value":"43IFALKW","created_at":"2026-07-04T15:29:30Z"}],"graph_snapshots":[{"event_id":"sha256:9d6eafe0fe9f297c4933b1e07de1fc14ddfbffdbd44049d52800fde13d092a25","target":"graph","created_at":"2026-07-04T15:29:30Z","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/9509079/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The lower moments of the unpolarized and polarized deep-inelastic structure functions of the nucleon are calculated on the lattice. The calculation is done with Wilson fermions and for three values of the hopping parameter $\\kappa$, so that we can perform the extrapolation to the chiral limit. Particular emphasis is put on the renormalization of lattice operators. The renormalization constants, which lead us from lattice to continuum operators, are computed perturbatively to one loop order as well as non-perturbatively.","authors_text":"A. Schiller, E.-M. Ilgenfritz, G. Schierholz, H. Oelrich, H. Perlt, M. G\\\"ockeler, P. Rakow, R. Horsley","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"1995-09-25T13:54:33Z","title":"A Lattice Evaluation of the Deep-Inelastic Structure Functions of the Nucleon"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9509079","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:b255933750d458b2deaa0fd139763a967a47e03ff5074d1b0f8655e14cee8b80","target":"record","created_at":"2026-07-04T15:29:30Z","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":"e6245a77a0b39d97df7a152ab8124ab24ac59a95c8fdea02007c4db3750fc4a3","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-lat","submitted_at":"1995-09-25T13:54:33Z","title_canon_sha256":"ae531faca9fefd4bc5b044ab7da00cc2e1909fb5d10bd7574a9b838240afd20c"},"schema_version":"1.0","source":{"id":"hep-lat/9509079","kind":"arxiv","version":1}},"canonical_sha256":"e6d0502d56132e9ecdcf65677a3d51aadae655b0c2c1cc3b7496d40cf2c1c862","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e6d0502d56132e9ecdcf65677a3d51aadae655b0c2c1cc3b7496d40cf2c1c862","first_computed_at":"2026-07-04T15:29:30.543151Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:29:30.543151Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"llazbUWM0BJ2h5dRmiKVRiIWEvf+Dq+FrmEyxnPPAFBM8MP1oDfbQOXeGgjxnbuCH0RX7mF5YMoCnRYTK9rSBA==","signature_status":"signed_v1","signed_at":"2026-07-04T15:29:30.543567Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/9509079","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b255933750d458b2deaa0fd139763a967a47e03ff5074d1b0f8655e14cee8b80","sha256:9d6eafe0fe9f297c4933b1e07de1fc14ddfbffdbd44049d52800fde13d092a25"],"state_sha256":"063f21c4d6e4da6d9c56d0850443b085327f415777e7d46804cb96d35fb9204c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dmjfU2BBa4IyzrauLc/Kps1urQ/HDxA+Un4vy1Z5cOM5Fwt+vn6GvPjusuIfjSXXCK8wJ5Z8suxk3jnRartCAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-06T20:20:44.453117Z","bundle_sha256":"280dafdc0ee2f34353ed85b6644c26d8698038c161d26ca2805271c44f5ce3fa"}}