{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:NA4CLCZOW3BQW6AVHYZO3HKBW7","short_pith_number":"pith:NA4CLCZO","schema_version":"1.0","canonical_sha256":"6838258b2eb6c30b78153e32ed9d41b7ffa65f002c3dd936cfdbc0653ea2f981","source":{"kind":"arxiv","id":"hep-lat/0001028","version":1},"attestation_state":"computed","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."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"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"},"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"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0001028","created_at":"2026-07-04T16:19:52.688832+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0001028v1","created_at":"2026-07-04T16:19:52.688832+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0001028","created_at":"2026-07-04T16:19:52.688832+00:00"},{"alias_kind":"pith_short_12","alias_value":"NA4CLCZOW3BQ","created_at":"2026-07-04T16:19:52.688832+00:00"},{"alias_kind":"pith_short_16","alias_value":"NA4CLCZOW3BQW6AV","created_at":"2026-07-04T16:19:52.688832+00:00"},{"alias_kind":"pith_short_8","alias_value":"NA4CLCZO","created_at":"2026-07-04T16:19:52.688832+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7","json":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7.json","graph_json":"https://pith.science/api/pith-number/NA4CLCZOW3BQW6AVHYZO3HKBW7/graph.json","events_json":"https://pith.science/api/pith-number/NA4CLCZOW3BQW6AVHYZO3HKBW7/events.json","paper":"https://pith.science/paper/NA4CLCZO"},"agent_actions":{"view_html":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7","download_json":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7.json","view_paper":"https://pith.science/paper/NA4CLCZO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0001028&json=true","fetch_graph":"https://pith.science/api/pith-number/NA4CLCZOW3BQW6AVHYZO3HKBW7/graph.json","fetch_events":"https://pith.science/api/pith-number/NA4CLCZOW3BQW6AVHYZO3HKBW7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7/action/storage_attestation","attest_author":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7/action/author_attestation","sign_citation":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7/action/citation_signature","submit_replication":"https://pith.science/pith/NA4CLCZOW3BQW6AVHYZO3HKBW7/action/replication_record"}},"created_at":"2026-07-04T16:19:52.688832+00:00","updated_at":"2026-07-04T16:19:52.688832+00:00"}