{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:WFCRFSDWG2LGNFEGFJ5R2H7UHZ","short_pith_number":"pith:WFCRFSDW","schema_version":"1.0","canonical_sha256":"b14512c87636966694862a7b1d1ff43e5d74f4e4839105bc25fbff0031c81dd4","source":{"kind":"arxiv","id":"hep-lat/0201018","version":1},"attestation_state":"computed","paper":{"title":"Monopoles in Lattice QCD with Abelian Projection as Quantum Monopoles","license":"","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"D. Singleton, V. Dzhunushaliev","submitted_at":"2002-01-22T02:59:54Z","abstract_excerpt":"Within the context of the Abelian Projection of QCD monopole-like quantum excitations of gauge fields are studied. We start with certain classical solutions, of the SU(2) Yang-Mills field equations, which are not monopole-like and whose energy density diverges as $r \\to \\infty$. These divergent classical solutions are then quantized using a modified version of Heisenberg's quantization technique for strongly interacting, nonlinear fields. The modified Heisenberg quantization technique leads to a system of equations with mixed quantum and classical degrees of freedom. By applying a Feynman path"},"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/0201018","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2002-01-22T02:59:54Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"75b3e00fd9ca57f84a53043ffa7be3392947ac76e14f179180b0c2ee8c50dc6f","abstract_canon_sha256":"16294b29440ea3963fc019c35e69ca4e2e58441ae8a8bbd608fbcfcb2a9b5aa0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:37:20.527179Z","signature_b64":"che9N8KnR5nlEFa7vSaDi8JiJHNJt2ePYl9rgKKBbfFhAzswRG1O9WR8OBoqNxqbBAiz+C7nbcjQqEZxhYOMDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b14512c87636966694862a7b1d1ff43e5d74f4e4839105bc25fbff0031c81dd4","last_reissued_at":"2026-05-18T02:37:20.526714Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:37:20.526714Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Monopoles in Lattice QCD with Abelian Projection as Quantum Monopoles","license":"","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"D. Singleton, V. Dzhunushaliev","submitted_at":"2002-01-22T02:59:54Z","abstract_excerpt":"Within the context of the Abelian Projection of QCD monopole-like quantum excitations of gauge fields are studied. We start with certain classical solutions, of the SU(2) Yang-Mills field equations, which are not monopole-like and whose energy density diverges as $r \\to \\infty$. These divergent classical solutions are then quantized using a modified version of Heisenberg's quantization technique for strongly interacting, nonlinear fields. The modified Heisenberg quantization technique leads to a system of equations with mixed quantum and classical degrees of freedom. By applying a Feynman path"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0201018","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":""},"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/0201018","created_at":"2026-05-18T02:37:20.526790+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0201018v1","created_at":"2026-05-18T02:37:20.526790+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0201018","created_at":"2026-05-18T02:37:20.526790+00:00"},{"alias_kind":"pith_short_12","alias_value":"WFCRFSDWG2LG","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_16","alias_value":"WFCRFSDWG2LGNFEG","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_8","alias_value":"WFCRFSDW","created_at":"2026-05-18T12:25:51.375804+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/WFCRFSDWG2LGNFEGFJ5R2H7UHZ","json":"https://pith.science/pith/WFCRFSDWG2LGNFEGFJ5R2H7UHZ.json","graph_json":"https://pith.science/api/pith-number/WFCRFSDWG2LGNFEGFJ5R2H7UHZ/graph.json","events_json":"https://pith.science/api/pith-number/WFCRFSDWG2LGNFEGFJ5R2H7UHZ/events.json","paper":"https://pith.science/paper/WFCRFSDW"},"agent_actions":{"view_html":"https://pith.science/pith/WFCRFSDWG2LGNFEGFJ5R2H7UHZ","download_json":"https://pith.science/pith/WFCRFSDWG2LGNFEGFJ5R2H7UHZ.json","view_paper":"https://pith.science/paper/WFCRFSDW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0201018&json=true","fetch_graph":"https://pith.science/api/pith-number/WFCRFSDWG2LGNFEGFJ5R2H7UHZ/graph.json","fetch_events":"https://pith.science/api/pith-number/WFCRFSDWG2LGNFEGFJ5R2H7UHZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WFCRFSDWG2LGNFEGFJ5R2H7UHZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WFCRFSDWG2LGNFEGFJ5R2H7UHZ/action/storage_attestation","attest_author":"https://pith.science/pith/WFCRFSDWG2LGNFEGFJ5R2H7UHZ/action/author_attestation","sign_citation":"https://pith.science/pith/WFCRFSDWG2LGNFEGFJ5R2H7UHZ/action/citation_signature","submit_replication":"https://pith.science/pith/WFCRFSDWG2LGNFEGFJ5R2H7UHZ/action/replication_record"}},"created_at":"2026-05-18T02:37:20.526790+00:00","updated_at":"2026-05-18T02:37:20.526790+00:00"}