{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2000:NA4CLCZOW3BQW6AVHYZO3HKBW7","short_pith_number":"pith:NA4CLCZO","canonical_record":{"source":{"id":"hep-lat/0001028","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2000-01-25T15:49:06Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"b9444e06f85c29ece10f8b9a891ca6a0b6e2f1461f7832ca9a6b8e96a7bb2576","abstract_canon_sha256":"2487ff877a560ec46880f58bc60a7b50fc29aca368a1234e5b62663209e01352"},"schema_version":"1.0"},"canonical_sha256":"6838258b2eb6c30b78153e32ed9d41b7ffa65f002c3dd936cfdbc0653ea2f981","source":{"kind":"arxiv","id":"hep-lat/0001028","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0001028","created_at":"2026-07-04T16:19:52Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0001028v1","created_at":"2026-07-04T16:19:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0001028","created_at":"2026-07-04T16:19:52Z"},{"alias_kind":"pith_short_12","alias_value":"NA4CLCZOW3BQ","created_at":"2026-07-04T16:19:52Z"},{"alias_kind":"pith_short_16","alias_value":"NA4CLCZOW3BQW6AV","created_at":"2026-07-04T16:19:52Z"},{"alias_kind":"pith_short_8","alias_value":"NA4CLCZO","created_at":"2026-07-04T16:19:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2000:NA4CLCZOW3BQW6AVHYZO3HKBW7","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0001028","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2000-01-25T15:49:06Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"b9444e06f85c29ece10f8b9a891ca6a0b6e2f1461f7832ca9a6b8e96a7bb2576","abstract_canon_sha256":"2487ff877a560ec46880f58bc60a7b50fc29aca368a1234e5b62663209e01352"},"schema_version":"1.0"},"canonical_sha256":"6838258b2eb6c30b78153e32ed9d41b7ffa65f002c3dd936cfdbc0653ea2f981","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:19:52.689191Z","signature_b64":"xJvGPmvrxGQIXBEGssi25KqRWRIYtkC9k07/120UBrewli8mVbjcMtFC817R3pLKc9N+8mUqwK/I7UBKV/RRBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6838258b2eb6c30b78153e32ed9d41b7ffa65f002c3dd936cfdbc0653ea2f981","last_reissued_at":"2026-07-04T16:19:52.688775Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:19:52.688775Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0001028","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":"2026-07-04T16:19:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yPezrlzVFrZmxr8ztmDYlrIJ0/2/CPEsQvn+VQMhkuRKFBhsZ4Xj8h1pAfcCeKjQmKkToMFQqtyxz2QiQuVODg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-06T06:11:46.951738Z"},"content_sha256":"cc954c115f0c3ce91dbf1937cd5622d5293b4fb20f71f2633dbc983fc861996e","schema_version":"1.0","event_id":"sha256:cc954c115f0c3ce91dbf1937cd5622d5293b4fb20f71f2633dbc983fc861996e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2000:NA4CLCZOW3BQW6AVHYZO3HKBW7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Towards a Many-Body Treatment of Hamiltonian Lattice SU(N) Gauge Theory","license":"","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"N.E. Ligterink, N.R. Walet, R.F. Bishop","submitted_at":"2000-01-25T15:49:06Z","abstract_excerpt":"We develop a consistent approach to Hamiltonian lattice gauge theory, using the maximal-tree gauge. The various constraints are discussed and implemented. An independent and complete set of variables for the colourless sector is determined. A general scheme to construct the eigenstates of the electric energy operator using a symbolic method is described. It is shown how the one-plaquette problem can be mapped onto a N-fermion problem. Explicit solutions for U(1), SU(2), SU(3), SU(4), and SU(5) lattice gauge theory are shown."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0001028","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/0001028/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":"2026-07-04T16:19:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mqKSmAGfPrg+Q+jpBxf+7Z6iYsVjZ248kNkMl7dr/k7Rgp4SDYNpL+WNxSi+Otj1F5rqu4VYaXj4Z26sAj7iCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-06T06:11:46.952105Z"},"content_sha256":"74e8e41c9361619b52546defc2af542096e8a8a2b953348c9170ddea2e30ffea","schema_version":"1.0","event_id":"sha256:74e8e41c9361619b52546defc2af542096e8a8a2b953348c9170ddea2e30ffea"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7/bundle.json","state_url":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7/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":"2026-07-06T06:11:46Z","links":{"resolver":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7","bundle":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7/bundle.json","state":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2000:NA4CLCZOW3BQW6AVHYZO3HKBW7","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":"2487ff877a560ec46880f58bc60a7b50fc29aca368a1234e5b62663209e01352","cross_cats_sorted":["hep-ph","hep-th"],"license":"","primary_cat":"hep-lat","submitted_at":"2000-01-25T15:49:06Z","title_canon_sha256":"b9444e06f85c29ece10f8b9a891ca6a0b6e2f1461f7832ca9a6b8e96a7bb2576"},"schema_version":"1.0","source":{"id":"hep-lat/0001028","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0001028","created_at":"2026-07-04T16:19:52Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0001028v1","created_at":"2026-07-04T16:19:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0001028","created_at":"2026-07-04T16:19:52Z"},{"alias_kind":"pith_short_12","alias_value":"NA4CLCZOW3BQ","created_at":"2026-07-04T16:19:52Z"},{"alias_kind":"pith_short_16","alias_value":"NA4CLCZOW3BQW6AV","created_at":"2026-07-04T16:19:52Z"},{"alias_kind":"pith_short_8","alias_value":"NA4CLCZO","created_at":"2026-07-04T16:19:52Z"}],"graph_snapshots":[{"event_id":"sha256:74e8e41c9361619b52546defc2af542096e8a8a2b953348c9170ddea2e30ffea","target":"graph","created_at":"2026-07-04T16:19:52Z","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/0001028/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We develop a consistent approach to Hamiltonian lattice gauge theory, using the maximal-tree gauge. The various constraints are discussed and implemented. An independent and complete set of variables for the colourless sector is determined. A general scheme to construct the eigenstates of the electric energy operator using a symbolic method is described. It is shown how the one-plaquette problem can be mapped onto a N-fermion problem. Explicit solutions for U(1), SU(2), SU(3), SU(4), and SU(5) lattice gauge theory are shown.","authors_text":"N.E. Ligterink, N.R. Walet, R.F. Bishop","cross_cats":["hep-ph","hep-th"],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2000-01-25T15:49:06Z","title":"Towards a Many-Body Treatment of Hamiltonian Lattice SU(N) Gauge Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0001028","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:cc954c115f0c3ce91dbf1937cd5622d5293b4fb20f71f2633dbc983fc861996e","target":"record","created_at":"2026-07-04T16:19:52Z","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":"2487ff877a560ec46880f58bc60a7b50fc29aca368a1234e5b62663209e01352","cross_cats_sorted":["hep-ph","hep-th"],"license":"","primary_cat":"hep-lat","submitted_at":"2000-01-25T15:49:06Z","title_canon_sha256":"b9444e06f85c29ece10f8b9a891ca6a0b6e2f1461f7832ca9a6b8e96a7bb2576"},"schema_version":"1.0","source":{"id":"hep-lat/0001028","kind":"arxiv","version":1}},"canonical_sha256":"6838258b2eb6c30b78153e32ed9d41b7ffa65f002c3dd936cfdbc0653ea2f981","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6838258b2eb6c30b78153e32ed9d41b7ffa65f002c3dd936cfdbc0653ea2f981","first_computed_at":"2026-07-04T16:19:52.688775Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:19:52.688775Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xJvGPmvrxGQIXBEGssi25KqRWRIYtkC9k07/120UBrewli8mVbjcMtFC817R3pLKc9N+8mUqwK/I7UBKV/RRBA==","signature_status":"signed_v1","signed_at":"2026-07-04T16:19:52.689191Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0001028","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cc954c115f0c3ce91dbf1937cd5622d5293b4fb20f71f2633dbc983fc861996e","sha256:74e8e41c9361619b52546defc2af542096e8a8a2b953348c9170ddea2e30ffea"],"state_sha256":"82560c89e1a42f8912692dbfba43dffe1f2c4884f1f251d294ca90f91f3dc1e1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wmZ52OeeJFbUhwwvmHirHEw7OdO1R+jCKrlhXbcHEJQnVSF5kOIsHeuzQNbLHHg4kLhtCiWV+NbYKbTuvIuiBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-06T06:11:46.953996Z","bundle_sha256":"add696898ca4fb55abee7953db234f53ebeafd9b7e512da839398db8d330e22f"}}