{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:5GZNUC3Y7SN2TPX6BFHAJYO2FE","short_pith_number":"pith:5GZNUC3Y","schema_version":"1.0","canonical_sha256":"e9b2da0b78fc9ba9befe094e04e1da2906cf5bb9b318d1aee9e414a82249bcf7","source":{"kind":"arxiv","id":"hep-lat/0508004","version":1},"attestation_state":"computed","paper":{"title":"Vacuum type of SU(2) gluodynamics in maximally Abelian and Landau gauges","license":"","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"Katsuya Ishiguro, M. I. Polikarpov, M. N. Chernodub, Toru Sekido, Tsuneo Suzuki, V. I. Zakharov, Yoshifumi Nakamura, Yoshihiro Mori","submitted_at":"2005-08-02T16:57:00Z","abstract_excerpt":"The vacuum type of SU(2) gluodynamics is studied using Monte-Carlo simulations in maximally Abelian (MA) gauge and in Landau (LA) gauge, where the dual Meissner effect is observed to work. The dual Meissner effect is characterized by the coherence and the penetration lengths. Correlations between Wilson loops and electric fields are evaluated in order to measure the penetration length in both gauges. The coherence length is shown to be fixed in the MA gauge from measurements of the monopole density around the static quark-antiquark pair. It is also shown numerically that a dimension 2 gluon op"},"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/0508004","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-08-02T16:57:00Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"55b1755118e7d471b0c3dd24586c5499d28c2688e5add3db031159a72f7319ca","abstract_canon_sha256":"cafbbe48e512e9de5c0bcc9fba7a36cae8b21d30025b2083b32d5300662fa6b5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:55:25.196979Z","signature_b64":"2MYE6/B8HCi2WaeVB33JWyi+0Cy1c/8tc10VuoXCjhNsrvz7Sc/wxL3/rKydna3hIfQo2jbr4ErZDaY9o+lUAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e9b2da0b78fc9ba9befe094e04e1da2906cf5bb9b318d1aee9e414a82249bcf7","last_reissued_at":"2026-07-04T16:55:25.196638Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:55:25.196638Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Vacuum type of SU(2) gluodynamics in maximally Abelian and Landau gauges","license":"","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"Katsuya Ishiguro, M. I. Polikarpov, M. N. Chernodub, Toru Sekido, Tsuneo Suzuki, V. I. Zakharov, Yoshifumi Nakamura, Yoshihiro Mori","submitted_at":"2005-08-02T16:57:00Z","abstract_excerpt":"The vacuum type of SU(2) gluodynamics is studied using Monte-Carlo simulations in maximally Abelian (MA) gauge and in Landau (LA) gauge, where the dual Meissner effect is observed to work. The dual Meissner effect is characterized by the coherence and the penetration lengths. Correlations between Wilson loops and electric fields are evaluated in order to measure the penetration length in both gauges. The coherence length is shown to be fixed in the MA gauge from measurements of the monopole density around the static quark-antiquark pair. It is also shown numerically that a dimension 2 gluon op"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0508004","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/0508004/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/0508004","created_at":"2026-07-04T16:55:25.196700+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0508004v1","created_at":"2026-07-04T16:55:25.196700+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0508004","created_at":"2026-07-04T16:55:25.196700+00:00"},{"alias_kind":"pith_short_12","alias_value":"5GZNUC3Y7SN2","created_at":"2026-07-04T16:55:25.196700+00:00"},{"alias_kind":"pith_short_16","alias_value":"5GZNUC3Y7SN2TPX6","created_at":"2026-07-04T16:55:25.196700+00:00"},{"alias_kind":"pith_short_8","alias_value":"5GZNUC3Y","created_at":"2026-07-04T16:55:25.196700+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.14902","citing_title":"Machine Learning Insights into Quark-Antiquark Interactions: Probing Field Distributions and String Tension in QCD","ref_index":58,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5GZNUC3Y7SN2TPX6BFHAJYO2FE","json":"https://pith.science/pith/5GZNUC3Y7SN2TPX6BFHAJYO2FE.json","graph_json":"https://pith.science/api/pith-number/5GZNUC3Y7SN2TPX6BFHAJYO2FE/graph.json","events_json":"https://pith.science/api/pith-number/5GZNUC3Y7SN2TPX6BFHAJYO2FE/events.json","paper":"https://pith.science/paper/5GZNUC3Y"},"agent_actions":{"view_html":"https://pith.science/pith/5GZNUC3Y7SN2TPX6BFHAJYO2FE","download_json":"https://pith.science/pith/5GZNUC3Y7SN2TPX6BFHAJYO2FE.json","view_paper":"https://pith.science/paper/5GZNUC3Y","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0508004&json=true","fetch_graph":"https://pith.science/api/pith-number/5GZNUC3Y7SN2TPX6BFHAJYO2FE/graph.json","fetch_events":"https://pith.science/api/pith-number/5GZNUC3Y7SN2TPX6BFHAJYO2FE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5GZNUC3Y7SN2TPX6BFHAJYO2FE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5GZNUC3Y7SN2TPX6BFHAJYO2FE/action/storage_attestation","attest_author":"https://pith.science/pith/5GZNUC3Y7SN2TPX6BFHAJYO2FE/action/author_attestation","sign_citation":"https://pith.science/pith/5GZNUC3Y7SN2TPX6BFHAJYO2FE/action/citation_signature","submit_replication":"https://pith.science/pith/5GZNUC3Y7SN2TPX6BFHAJYO2FE/action/replication_record"}},"created_at":"2026-07-04T16:55:25.196700+00:00","updated_at":"2026-07-04T16:55:25.196700+00:00"}