{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:WYMVBX3HA236LK5SXRPO2MYBFN","short_pith_number":"pith:WYMVBX3H","schema_version":"1.0","canonical_sha256":"b61950df6706b7e5abb2bc5eed33012b4920b20ca3b4c6102c8b72e2d23dd3d4","source":{"kind":"arxiv","id":"hep-th/0604185","version":2},"attestation_state":"computed","paper":{"title":"On pure Yang-Mills theory in 3+1 dimensions: Hamiltonian, vacuum and gauge invariant variables","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Laurent Freidel","submitted_at":"2006-04-25T09:44:19Z","abstract_excerpt":"In this work we discuss an analytic approach towards the solution of pure Yang-Mills theory in 3+1 dimensional spacetime which strongly suggests that the recent strategy already applied to pure Yang-Mills theory in 2+1 can be extended to 3+1 dimensions. We show that the local gauge invariant variables introduced by Bars gives a natural generalisation to any dimension of the formalism of Karabali and Nair which recently led to a new understanding of the physics of QCD in dimension 2+1. After discussing the kinematics of these variables, we compute the jacobian between the Yang-Mills and Bars va"},"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-th/0604185","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2006-04-25T09:44:19Z","cross_cats_sorted":[],"title_canon_sha256":"d8db6439d08da0ca9cb1075dca4779eb94d81a68daf3158651fdf527f708c020","abstract_canon_sha256":"e56b055c0adde8eace9e7ed553d02fc88c6d2356ff18f4f8f287dbcd1304c330"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:54:32.698297Z","signature_b64":"1R/ZEjG+z7YvGXoyg4OFMbSJiHH4x3+QvOCEGefMf2QYth7mweqCEDSZUvInbGYlwvi33VIfN9Q1JC7PyawyDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b61950df6706b7e5abb2bc5eed33012b4920b20ca3b4c6102c8b72e2d23dd3d4","last_reissued_at":"2026-07-04T14:54:32.697945Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:54:32.697945Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On pure Yang-Mills theory in 3+1 dimensions: Hamiltonian, vacuum and gauge invariant variables","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Laurent Freidel","submitted_at":"2006-04-25T09:44:19Z","abstract_excerpt":"In this work we discuss an analytic approach towards the solution of pure Yang-Mills theory in 3+1 dimensional spacetime which strongly suggests that the recent strategy already applied to pure Yang-Mills theory in 2+1 can be extended to 3+1 dimensions. We show that the local gauge invariant variables introduced by Bars gives a natural generalisation to any dimension of the formalism of Karabali and Nair which recently led to a new understanding of the physics of QCD in dimension 2+1. After discussing the kinematics of these variables, we compute the jacobian between the Yang-Mills and Bars va"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0604185","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-th/0604185/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-th/0604185","created_at":"2026-07-04T14:54:32.698009+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0604185v2","created_at":"2026-07-04T14:54:32.698009+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0604185","created_at":"2026-07-04T14:54:32.698009+00:00"},{"alias_kind":"pith_short_12","alias_value":"WYMVBX3HA236","created_at":"2026-07-04T14:54:32.698009+00:00"},{"alias_kind":"pith_short_16","alias_value":"WYMVBX3HA236LK5S","created_at":"2026-07-04T14:54:32.698009+00:00"},{"alias_kind":"pith_short_8","alias_value":"WYMVBX3H","created_at":"2026-07-04T14:54:32.698009+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/WYMVBX3HA236LK5SXRPO2MYBFN","json":"https://pith.science/pith/WYMVBX3HA236LK5SXRPO2MYBFN.json","graph_json":"https://pith.science/api/pith-number/WYMVBX3HA236LK5SXRPO2MYBFN/graph.json","events_json":"https://pith.science/api/pith-number/WYMVBX3HA236LK5SXRPO2MYBFN/events.json","paper":"https://pith.science/paper/WYMVBX3H"},"agent_actions":{"view_html":"https://pith.science/pith/WYMVBX3HA236LK5SXRPO2MYBFN","download_json":"https://pith.science/pith/WYMVBX3HA236LK5SXRPO2MYBFN.json","view_paper":"https://pith.science/paper/WYMVBX3H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0604185&json=true","fetch_graph":"https://pith.science/api/pith-number/WYMVBX3HA236LK5SXRPO2MYBFN/graph.json","fetch_events":"https://pith.science/api/pith-number/WYMVBX3HA236LK5SXRPO2MYBFN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WYMVBX3HA236LK5SXRPO2MYBFN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WYMVBX3HA236LK5SXRPO2MYBFN/action/storage_attestation","attest_author":"https://pith.science/pith/WYMVBX3HA236LK5SXRPO2MYBFN/action/author_attestation","sign_citation":"https://pith.science/pith/WYMVBX3HA236LK5SXRPO2MYBFN/action/citation_signature","submit_replication":"https://pith.science/pith/WYMVBX3HA236LK5SXRPO2MYBFN/action/replication_record"}},"created_at":"2026-07-04T14:54:32.698009+00:00","updated_at":"2026-07-04T14:54:32.698009+00:00"}