{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:YUWF53MV3U57KWJDAVHSCONZIJ","short_pith_number":"pith:YUWF53MV","schema_version":"1.0","canonical_sha256":"c52c5eed95dd3bf55923054f2139b9425f06489416041798d2468a80e95fea16","source":{"kind":"arxiv","id":"1101.5098","version":1},"attestation_state":"computed","paper":{"title":"Hamiltonian approach to Yang-Mills theory in Coulomb gauge - revisited","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-th","authors_text":"A. Weber, D. R. Campagnari, G. Burgio, H. Reinhardt, J. M. Pawlowski, M. Leder, M. Quandt","submitted_at":"2011-01-26T16:18:20Z","abstract_excerpt":"I briefly review results obtained within the variational Hamiltonian approach to Yang-Mills theory in Coulomb gauge and confront them with recent lattice data. The variational approach is extended to non-Gaussian wave functionals including three- and four-gluon kernels in the exponential of the vacuum wave functional and used to calculate the three-gluon vertex. A new functional renormalization group flow equation for Hamiltonian Yang--Mills theory in Coulomb gauge is solved for the gluon and ghost propagator under the assumption of ghost dominance. The results are compared to those obtained i"},"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":"1101.5098","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-01-26T16:18:20Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"6e4fa88ad72d7819b9877e0c0cade9ce02c03a6dac26ef9e666791f71c7e233c","abstract_canon_sha256":"cb00ec72137c8fca993e67bb1fe369864dd216113dcce4c8033c9a3d54746b3d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:03:21.917099Z","signature_b64":"3qk50ba0fQNlp8VfGHAzU2DogBQ0JaDqHj7UYZFYU+UbiwFeyIXB6Kww91etXkQu8HXHRGG+/UMzFzLb7VC2DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c52c5eed95dd3bf55923054f2139b9425f06489416041798d2468a80e95fea16","last_reissued_at":"2026-05-18T02:03:21.916351Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:03:21.916351Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hamiltonian approach to Yang-Mills theory in Coulomb gauge - revisited","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-th","authors_text":"A. Weber, D. R. Campagnari, G. Burgio, H. Reinhardt, J. M. Pawlowski, M. Leder, M. Quandt","submitted_at":"2011-01-26T16:18:20Z","abstract_excerpt":"I briefly review results obtained within the variational Hamiltonian approach to Yang-Mills theory in Coulomb gauge and confront them with recent lattice data. The variational approach is extended to non-Gaussian wave functionals including three- and four-gluon kernels in the exponential of the vacuum wave functional and used to calculate the three-gluon vertex. A new functional renormalization group flow equation for Hamiltonian Yang--Mills theory in Coulomb gauge is solved for the gluon and ghost propagator under the assumption of ghost dominance. The results are compared to those obtained i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.5098","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":"1101.5098","created_at":"2026-05-18T02:03:21.916472+00:00"},{"alias_kind":"arxiv_version","alias_value":"1101.5098v1","created_at":"2026-05-18T02:03:21.916472+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1101.5098","created_at":"2026-05-18T02:03:21.916472+00:00"},{"alias_kind":"pith_short_12","alias_value":"YUWF53MV3U57","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_16","alias_value":"YUWF53MV3U57KWJD","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_8","alias_value":"YUWF53MV","created_at":"2026-05-18T12:26:47.523578+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/YUWF53MV3U57KWJDAVHSCONZIJ","json":"https://pith.science/pith/YUWF53MV3U57KWJDAVHSCONZIJ.json","graph_json":"https://pith.science/api/pith-number/YUWF53MV3U57KWJDAVHSCONZIJ/graph.json","events_json":"https://pith.science/api/pith-number/YUWF53MV3U57KWJDAVHSCONZIJ/events.json","paper":"https://pith.science/paper/YUWF53MV"},"agent_actions":{"view_html":"https://pith.science/pith/YUWF53MV3U57KWJDAVHSCONZIJ","download_json":"https://pith.science/pith/YUWF53MV3U57KWJDAVHSCONZIJ.json","view_paper":"https://pith.science/paper/YUWF53MV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1101.5098&json=true","fetch_graph":"https://pith.science/api/pith-number/YUWF53MV3U57KWJDAVHSCONZIJ/graph.json","fetch_events":"https://pith.science/api/pith-number/YUWF53MV3U57KWJDAVHSCONZIJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YUWF53MV3U57KWJDAVHSCONZIJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YUWF53MV3U57KWJDAVHSCONZIJ/action/storage_attestation","attest_author":"https://pith.science/pith/YUWF53MV3U57KWJDAVHSCONZIJ/action/author_attestation","sign_citation":"https://pith.science/pith/YUWF53MV3U57KWJDAVHSCONZIJ/action/citation_signature","submit_replication":"https://pith.science/pith/YUWF53MV3U57KWJDAVHSCONZIJ/action/replication_record"}},"created_at":"2026-05-18T02:03:21.916472+00:00","updated_at":"2026-05-18T02:03:21.916472+00:00"}