{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:D7QJWLIJU5L6N4YUSIQDFRS5U6","short_pith_number":"pith:D7QJWLIJ","schema_version":"1.0","canonical_sha256":"1fe09b2d09a757e6f314922032c65da7b3a43ebc8e70a52d07cad16d5cdfb02a","source":{"kind":"arxiv","id":"hep-lat/9605001","version":2},"attestation_state":"computed","paper":{"title":"Improved Hamiltonian for Minkowski Yang-Mills Theory","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Guy D. Moore","submitted_at":"1996-05-01T06:08:56Z","abstract_excerpt":"I develop an improved Hamiltonian for classical, Minkowski Yang-Mills theory, which evolves infrared fields with corrections from lattice spacing $a$ beginning at $O(a^4)$. I use it to investigate the response of Chern-Simons number to a chemical potential, and to compute the maximal Lyapunov exponent. Both quantities have small $a$ limits, in both cases within $10\\% $ of the limit found using the unimproved (Kogut Susskind) Hamiltonian. For the maximal Lyapunov exponent the limits differ by about $5 \\% $, significant at about $5 \\sigma$, indicating that while a small $a$ limit exists, its val"},"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/9605001","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1996-05-01T06:08:56Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"f1ab35fdc0e28061b5f10257fe1e826c5ad713309143a6c7c94dd31dcbeb53f7","abstract_canon_sha256":"04d45da1c14b1a07f5973178977bd0e0dabb703ac3cc65006014f0099d1652eb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:01:21.643970Z","signature_b64":"rE7r4hiqHuAwr9iZkZsKWQi0DdsdX+iTfhzjMGNc7isJNVi+OZY6PIjQwsm0Wa90cftqxFaikNx9fM+t8nQHCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1fe09b2d09a757e6f314922032c65da7b3a43ebc8e70a52d07cad16d5cdfb02a","last_reissued_at":"2026-07-04T16:01:21.643613Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:01:21.643613Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Improved Hamiltonian for Minkowski Yang-Mills Theory","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Guy D. Moore","submitted_at":"1996-05-01T06:08:56Z","abstract_excerpt":"I develop an improved Hamiltonian for classical, Minkowski Yang-Mills theory, which evolves infrared fields with corrections from lattice spacing $a$ beginning at $O(a^4)$. I use it to investigate the response of Chern-Simons number to a chemical potential, and to compute the maximal Lyapunov exponent. Both quantities have small $a$ limits, in both cases within $10\\% $ of the limit found using the unimproved (Kogut Susskind) Hamiltonian. For the maximal Lyapunov exponent the limits differ by about $5 \\% $, significant at about $5 \\sigma$, indicating that while a small $a$ limit exists, its val"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9605001","kind":"arxiv","version":2},"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/9605001/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/9605001","created_at":"2026-07-04T16:01:21.643680+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9605001v2","created_at":"2026-07-04T16:01:21.643680+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9605001","created_at":"2026-07-04T16:01:21.643680+00:00"},{"alias_kind":"pith_short_12","alias_value":"D7QJWLIJU5L6","created_at":"2026-07-04T16:01:21.643680+00:00"},{"alias_kind":"pith_short_16","alias_value":"D7QJWLIJU5L6N4YU","created_at":"2026-07-04T16:01:21.643680+00:00"},{"alias_kind":"pith_short_8","alias_value":"D7QJWLIJ","created_at":"2026-07-04T16:01:21.643680+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.12493","citing_title":"Symmetry-preserving neural networks in lattice field theories","ref_index":116,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/D7QJWLIJU5L6N4YUSIQDFRS5U6","json":"https://pith.science/pith/D7QJWLIJU5L6N4YUSIQDFRS5U6.json","graph_json":"https://pith.science/api/pith-number/D7QJWLIJU5L6N4YUSIQDFRS5U6/graph.json","events_json":"https://pith.science/api/pith-number/D7QJWLIJU5L6N4YUSIQDFRS5U6/events.json","paper":"https://pith.science/paper/D7QJWLIJ"},"agent_actions":{"view_html":"https://pith.science/pith/D7QJWLIJU5L6N4YUSIQDFRS5U6","download_json":"https://pith.science/pith/D7QJWLIJU5L6N4YUSIQDFRS5U6.json","view_paper":"https://pith.science/paper/D7QJWLIJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/9605001&json=true","fetch_graph":"https://pith.science/api/pith-number/D7QJWLIJU5L6N4YUSIQDFRS5U6/graph.json","fetch_events":"https://pith.science/api/pith-number/D7QJWLIJU5L6N4YUSIQDFRS5U6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/D7QJWLIJU5L6N4YUSIQDFRS5U6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/D7QJWLIJU5L6N4YUSIQDFRS5U6/action/storage_attestation","attest_author":"https://pith.science/pith/D7QJWLIJU5L6N4YUSIQDFRS5U6/action/author_attestation","sign_citation":"https://pith.science/pith/D7QJWLIJU5L6N4YUSIQDFRS5U6/action/citation_signature","submit_replication":"https://pith.science/pith/D7QJWLIJU5L6N4YUSIQDFRS5U6/action/replication_record"}},"created_at":"2026-07-04T16:01:21.643680+00:00","updated_at":"2026-07-04T16:01:21.643680+00:00"}